Dynamic ion-ion and water-ion interactions in ion channels.

The dynamic interactions among ions and water molecules in ion channels are treated based on an assumption that ions at binding sites can be knocked off by both transient entering ions and local water molecules. The theory, when applied to a single-site model K+ channel, provides solutions for super- and subsaturations, flux-ratio exponent (n') greater than 1, osmotic streaming current, activity-dependent reversal potentials, and anomalous mole-fraction behavior. The analysis predicts that: (a) the saturation may but, in general, does not follow the Michaelis-Menten relation; (b) streaming current results from imbalanced water-ion knock-off interactions; (c) n' greater than 1 even for single-site channels, but it is unlikely to exceed 1.4 unless the pore is occupied by one or more ion(s); (d) in the calculation involving two permeant ion species with similar radii, the heavier ions show higher affinity; the ion-ion knock-off dissociation from the site is more effective when two interacting ions are identical. Therefore, the "multi-ion behaviors" found in most ion channels are the consequences of dynamic ion-ion and water-ion interactions. The presence of these interactions does not require two or more binding sites in channels.     

Voltage-dependent slowing of K channel closing kinetics by Rb+

We have studied the effect of Rb+ on K channel closing kinetics in toadfish pancreatic islet cells. These channels are voltage dependent, activating at voltages positive to -10 mV. The channels also inactivate upon prolonged depolarizations, and the inactivation time course is best fit by the sum of two exponentials. Instantaneous current-voltage relationships show that external Rb+ enters the channel as easily as K+, but carries less current. In the voltage range from -140 to -50 mV, the closing time course of the channels can be fit with a single exponential. When Rb+ is present in the external solution the channels close more slowly. The magnitude of this Rb+ effect is voltage dependent, decreasing at more negative voltages. Similarly, when the internal solution contains Rb+ instead of K+ the closing time constants are increased. The effect of internal Rb+ is also voltage dependent; at voltages positive to -80 mV the closing time constant in internal Rb+ is slower than in K+, whereas at more negative voltages the difference is negligible. With internal Rb+, the relationship between the closing time constant and voltage is best fit with two exponential components, suggesting the presence of two distinct voltage-dependent processes. The results are discussed in terms of a model of the K channel with two internal binding sites, and we conclude that Rb+ produces its effects on channel gating by binding to a site in the pore.     

The multi-ion nature of the pore in Shaker K+ channels.

We have investigated some of the permeation properties of the pore in Shaker K channels. We determined the apparent permeability ratio of K+, Rb+, and NH4+ ions and block of the pore by external Cs+ ions. Shaker channels were expressed with the baculovirus/Sf9 expression system and the channel currents measured with the whole-cell variant of the patch clamp technique. The apparent permeability ratio, PRb/PK, determined in biionic conditions with internal K+, was a function of external Rb+ concentration. A large change in PRb/PK occurred with reversed ionic conditions (internal Rb+ and external K+). These changes in apparent permeability were not due to differences in membrane potential. With internal K+, PNH4/PK was not a function of external NH4+ concentration (at least over the range 50-120 mM). We also investigated block of the pore by external Cs+ ions. At a concentration of 20 mM, Cs+ block had a voltage dependence equivalent to that of an ion with a valence of 0.91; this increased to 1.3 at 40 mM Cs+. We show that a 4-barrier, 3-site permeation model can simulate these and many of the other known properties of ion permeation in Shaker channels.     

Voltage-activated ionic channels and conductances in embryonic chick osteoblast cultures

Patch-clamp measurements were made on osteoblast-like cells isolated from embryonic chick calvaria. Cell-attached-patch measurements revealed two types of high conductance (100-250 pS) channels, which rapidly activated upon 50-100 mV depolarization. One type showed sustained and the other transient activation over a 10-sec period of depolarization. The single-channel conductances of these channel types were about 100 or 250 pS, depending on whether the pipettes were filled with a low K+ (3 mM) or high K+ (143 mM) saline, respectively. The different reversal potentials under these conditions were consistent with at least K+ conduction. Whole-cell measurements revealed the existence of two types of outward rectifying conductances. The first type conducts K+ ions and activates within 20-200 msec (depending on the stimulus) upon depolarizing voltage steps from less than -60 mV to greater than -30 mV. It inactivates almost completely with a time constant of 2-3 sec. Recovery from inactivation is biphasic with an initial rapid phase (1-2 sec) followed by a slow phase (greater than 20 sec). The second whole-cell conductance activates at positive membrane potentials of greater than +50 mV. It also rapidly turns on upon depolarizing voltage steps. Activation may partly disappear at the higher voltages. Its single channels of 140 pS conductance were identified in the whole cell and did conduct K+ ions but were not highly Cl- or Na+ selective. The results show that osteoblasts may express various types of voltage controlled ionic channels. We predict a role for such channels in mineral metabolism of bone tissue and its control by osteoblasts.     

Contributions of a negatively charged residue in the hydrophobic domain of the IRK1 inwardly rectifying K+ channel to K(+)-selective permeation.

Inwardly rectifying K+ channels are highly selective for K+ ions and show strong interaction with ions in the pore. Both features are important for the physiological functions of these channels and pose intriguing mechanistic questions of ion permeation. The aspartate residue in the second putative transmembrane segment of the IRK1 inwardly rectifying K+ channel, previously implicated in inward rectification gating due to cytoplasmic Mg2+ and polyamine block, is found in this study to be crucial for the channel's ability to distinguish between K+ and Rb+ ions. Mutation of this residue also perturbs the interaction between the channel pore and the Sr2+ blocking ion. Our studies suggest that this aspartate residue contributes to a selectivity filter near the cytoplasmic end of the pore.     

Single ion occupancy and steady-state gating of Na channels in squid giant axon

The properties of the small fraction of tetrodotoxin (TTX)-sensitive Na channels that remain open in the steady state were studied in internally dialyzed voltage clamped squid giant axons. The observed Ussing flux ratio exponent (n') of 0.97 plus minus 0.03 (calculated from simultaneous measurements of TTX-sensitive current and (22)Na efflux) and nonindependent behavior of Na current at high internal [Na] are explained by a one-site ("1s") permeation model characterized by a single effective binding site within the channel pore in equilibrium with internal Na ions (apparent equilibrium dissociation constant K(Nai)(0) = 0.61 +/- 0.08 M). Steady-state open probability of the TTX-sensitive channels can be modeled by the product p(a)p(infinity), where p(a) represents voltage-dependent activation described by a Boltzmann distribution with midpoint V(a) = -7 mV and effective valence z(a) = 3.2 (Vandenberg, C.A., and F. Bezanilla. 1991. BIOPHYS: J. 60:1499--1510) coupled to voltage-independent inactivation by an equilibrium constant (Bezanilla, F., and C.M. Armstrong. 1977. J. Gen. Physiol. 70:549--566) K(eq) = 770. The factor p(infinity) represents voltage-dependent inactivation with empirical midpoint V(infinity)= -83 plus minus 5 mV and effective valence z(infinity) = 0.55 plus minus 0.03. The composite p(a)p(infinity)1s model describes the steady-state voltage dependence of the persistent TTX-sensitive current well.     

Dilated and defunct K channels in the absence of K+

Potassium ions are vital for maintaining functionality of K channels. In their absence, many K channel types enter a long-lasting defunct condition characterized by absence of conductance and drastic changes in gating current. We show that channels pass through a dilated condition with altered selectivity as they are becoming defunct. To characterize these abnormalities we examined gating and ionic currents generated by Shaker IR and by three nonconducting mutants, W434F, D447N, and Y445A, in 0 K+. On entering the dilated condition, Shaker IR becomes permeable to Na+ and tetramethylammonium-positive (TMA+), signaling deformation of the selectivity filter. When dilated, nearly normal closing is possible at -140 mV. At -80 mV, however, closing is very slow and channels stray from the dilated into the defunct condition. Restoration from defunct to dilated condition requires tens of seconds at 0 mV and can occur in the absence of K+. W434F and D447N are similar to Shaker IR, showing Na+ and TMA+ permeability when dilated. The defunct gating currents are similar in Shaker IR and these two mutants and are reminiscent of the early transitions of normal gating. Y445A does not become defunct and shows Na+ but not TMA+ permeability on K+ removal.     

Potassium channel activity recorded from the apical membrane of freshly isolated epithelial cells in rat caudal epididymis.

K+ channels were recorded in excised, inside-out patches from the apical membrane of the freshly isolated tubule of the caudal portion of the rat epididymis. With asymmetric K+ concentrations in bath and pipette (140 mM K+in/6 mM K+out), the channels had a slope conductance of 54.2 pS at 0 mV. The relative permeability of K+ over Na+ was about 171 to 1. The channels were activated by intracellular Ca2+ and by membrane depolarization. These channels belong to a class defined as "intermediate-conductance Ca2+-activated K+ channel. " External tetraethylammonium ions (TEA+) caused a flickery block of the channel with reduction in single-channel current amplitude measured at a range of holding membrane potentials (-40 to 60 mV). Activity of the K+ channels was inhibited by intracellular ATP (KD =1.188 mM). The channel activity was detected only occasionally in patches from the apical membrane (about 1 in 17 patches containing active channels). The presence of the intermediate-conductance Ca2+-activated K+ channels indicates that they could provide a route for K+ secretion in a Ca2+-dependent process responsible for a high luminal K+ concentration found in the epididymal duct of the rat.     

A unique voltage sensor sensitizes the potassium channel AKT2 to phosphoregulation

Among all voltage-gated K+ channels from the model plant Arabidopsis thaliana, the weakly rectifying K+ channel (K(weak) channel) AKT2 displays unique gating properties. AKT2 is exceptionally regulated by phosphorylation: when nonphosphorylated AKT2 behaves as an inward-rectifying potassium channel; phosphorylation of AKT2 abolishes inward rectification by shifting its activation threshold far positive (>200 mV) so that it closes only at voltages positive of +100 mV. In its phosphorylated form, AKT2 is thus locked in the open state in the entire physiological voltage range. To understand the molecular grounds of this unique gating behavior, we generated chimeras between AKT2 and the conventional inward-rectifying channel KAT1. The transfer of the pore from KAT1 to AKT2 altered the permeation properties of the channel. However, the gating properties were unaffected, suggesting that the pore region of AKT2 is not responsible for the unique K(weak) gating. Instead, a lysine residue in S4, highly conserved among all K(weak) channels but absent from other plant K+ channels, was pinpointed in a site-directed mutagenesis approach. Substitution of the lysine by serine or aspartate abolished the "open-lock" characteristic and converted AKT2 into an inward-rectifying channel. Interestingly, phosphoregulation of the mutant AKT2-K197S appeared to be similar to that of the K(in) channel KAT1: as suggested by mimicking the phosphorylated and dephosphorylated states, phosphorylation induced a shift of the activation threshold of AKT2-K197S by about +50 mV. We conclude that the lysine residue K197 sensitizes AKT2 to phosphoregulation. The phosphorylation-induced reduction of the activation energy in AKT2 is approximately 6 kT larger than in the K197S mutant. It is discussed that this hypersensitive response of AKT2 to phosphorylation equips a cell with the versatility to establish a potassium gradient and to make efficient use of it.     

Electrostatic domino effect in the Shaker K channel turret

Voltage-gated K channels are regulated by extracellular divalent cations such as Mg(2+) and Sr(2+), either by screening of fixed negative surface charges, by binding directly or close to the voltage sensor, or by binding to the pore. Different K channels display different sensitivity to divalent cations. For instance, 20 mM MgCl(2) shifts the conductance versus voltage curve, G(V), of the Kv1-type Shaker channel with 14 mV, while the G(V) of Kv2.1 is shifted only with 7 mV. This shift difference is paralleled with different working ranges. Kv1-type channels open at approximately -20 mV and Kv2.1 channel open at approximately +5 mV. The aim of this study was to identify critical residues for this Mg(2+)-induced G(V) shift by introducing Kv2.1 channel residues in the Shaker K channel. The K channels were expressed in Xenopus laevis oocytes and studied with the two-electrode voltage-clamp technique. We found that three neutral-to-positive amino-acid residue exchanges in the extracellular loops connecting transmembrane segments S5 and S6 transferred the Mg(2+)-shifting properties. The contributions of the three residues were additive, and thus independent of each other, with the contributions in the order 425 > 419 > 451. Charging 425 and 419 not only affect the Mg(2+)-induced G(V) shift with 5-6 mV, but also shifts the G(V) with 17 mV. Thus, a few strategically placed surface charges clearly modulate the channel's working range. Residue 425, located at some distance away from the voltage sensor, was shown to electrostatically affect residue K427, which in turn affects the voltage sensor S4-thus, an electrostatic domino effect.     

A calcium and ATP sensitive nonselective cation channel in the antiluminal membrane of rat cerebral capillary endothelial cells.

The patch-clamp technique was applied to the antiluminal membrane of freshly isolated capillaries of rat brain (blood-brain barrier). With 1.3 mM Ca2+ in the bath, excision of membrane patches evoked ion channels, which could not be observed in cell-attached mode. The channel was about equally permeable to Na+ and K+ ions, but not measurable permeable to Cl- and the divalent ions Ca2+ and Ba2+. The current-voltage curve was linear in the investigated voltage range (-80 mV to +80 mV), and the single-channel conductance was 31 +/- 2 pS (n = 22). The channel open probability was not dependent on the applied potential. Lowering of Ca2+ to 1 microM or below on the cytosolic side inactivated the channels, whereas addition of cytosolic ATP (1 mM) inhibited channel activity completely and reversibly. The channel was blocked by the inhibitor of nonselective cation channels in rat exocrine pancreas 3',5-dichlorodiphenylamine-2-carboxylic acid (DCDPC, 10 microM) and by the antiinflammatory drugs flufenamic acid (greater than 10 microM) and tenidap (100 microM), as well as by gadolinium (10 microM). Thus, these nonselective cation channels have many properties in common with similar channels observed in fluid secreting epithelia. The channel could be involved in the transport of K+ ions from brain to blood side.     

Two novel cardiac atrial K+ channels, IK.AA and IK.PC

Two K(+)-selective channels in neonatal rat atrial cells activated by lipophilic compounds have been characterized in detail. The arachidonic acid-stimulated channel (IK.AA) had a slope conductance of 124 +/- 17 pS at +30 mV in symmetrical 140 mM potassium and a mean open time of approximately 1 ms, and was relatively voltage independent. IK.AA activity was reversibly increased by lowering pH to 6.0. Arachidonic acid was most effective in activating this channel, although a number of lipophilic compounds resulted in activation. Surprisingly, choline, a polar molecule, also activated the channel. A second K+ channel was activated by 10 microM phosphatidylcholine applied to the intracellular surface of inside-out atrial patches. This channel (IK.PC) had a slope conductance of 60 +/- 6 pS at +40 mV and a mean open time of approximately 0.6 ms, and was also relatively voltage independent. Fatty acids are probably monomeric in the membrane under the conditions of our recording; thus detergent effects are unlikely. Since a number of compounds including fatty acids and prostaglandins activated these two channels, an indirect, channel-specific mechanism may account for activation of these two cardiac K+ channels.     

Probing of pore in the Chara gymnophylla K+ channel by blocking cations and by streaming potential measurements.

The current-voltage (I-V) relationship of single K+ channels present in the Chara gymnophylla droplet membrane was studied. The channel presumably contains large mouths at both pore ends which are sufficiently wide to accommodate TEA+ as evidenced by internal and external TEA+ blockade. The voltage dependence of blockade by external Cs+ and Na+ reveals the multi-ion occupancy of the channel. The value of streaming potential (4.0 mV/osmol) measured in the Chara K+ channel indicates that the channel contains up to nine water molecules in the narrow region. It is concluded that the length of this region is around 28 A.     

Calcium channel selectivity for divalent and monovalent cations. Voltage and concentration dependence of single channel current in ventricular heart cells

Single channel and whole cell recordings were used to study ion permeation through Ca channels in isolated ventricular heart cells of guinea pigs. We evaluated the permeability to various divalent and monovalent cations in two ways, by measuring either unitary current amplitude or reversal potential (Erev). According to whole cell measurements of Erev, the relative permeability sequence is Ca2+ greater than Sr2+ greater than Ba2+ for divalent ions; Mg2+ is not measurably permeant. Monovalent ions follow the sequence Li+ greater than Na+ greater than K+ greater than Cs+, and are much less permeant than the divalents. These whole cell measurements were supported by single channel recordings, which showed clear outward currents through single Ca channels at strong depolarizations, similar values of Erev, and similar inflections in the current-voltage relation near Erev. Information from Erev measurements stands in contrast to estimates of open channel flux or single channel conductance, which give the sequence Na+ (85 pS) greater than Li+ (45 pS) greater than Ba2+ (20 pS) greater than Ca2+ (9 pS) near 0 mV with 110-150 mM charge carrier. Thus, ions with a higher permeability, judged by Erev, have lower ion transfer rates. In another comparison, whole cell Na currents through Ca channels are halved by less than 2 microM [Ca]o, but greater than 10 mM [Ca]o is required to produce half-maximal unitary Ca current. All of these observations seem consistent with a recent hypothesis for the mechanism of Ca channel permeation, which proposes that: ions pass through the pore in single file, interacting with multiple binding sites along the way; selectivity is largely determined by ion affinity to the binding sites rather than by exclusion by a selectivity filter; occupancy by only one Ca ion is sufficient to block the pore's high conductance for monovalent ions like Na+; rapid permeation by Ca ions depends upon double occupancy, which only becomes significant at millimolar [Ca]o, because of electrostatic repulsion or some other interaction between ions; and once double occupancy occurs, the ion-ion interaction helps promote a quick exit of Ca ions from the pore into the cell.     

Streaming potential measurements in Ca2+-activated K+ channels from skeletal and smooth muscle. Coupling of ion and water fluxes.

Streaming potentials arising across large-conductance Ca2+-activated K+ channels incorporated into planar lipid bilayers were measured. Ca2+-activated channels obtained either from skeletal muscle or from smooth muscle membranes were used. Streaming potentials were extracted from the current-voltage relationship for the open channel obtained in the presence of an osmotic gradient. The osmotic gradient was established by adding glucose to one side of the membrane. At 300 mM KCl, the average streaming potential was 0.72 mV/osmol per kg for t-tubule channels and 0.83 mV/osmol per kg for smooth muscle channels. Streaming potential values depend on KCl concentration, they decrease as KCl concentration increases, and the value obtained by extrapolation to zero KCl concentration is 0.85 mV/osmol per kg. Assuming that water and ions cannot pass each other, at least in a region of the channel, the streaming potential values obtained indicate that this region contains a minimum of two and a maximum of four water molecules. It is concluded that the channel has a narrow region with a length of 0.6-1.2 nm.     

Modulation of the activity of Ca(2+)-activated K+ channels by internal Mg2+ in cultured kidney cells vero.

The inside-out mode of the patch-clamp method was used to study the effects of internal Mg2+ on single large-conductance (193+/-7 pS) Ca(2+)-activated K+ channels in cultured kidney cells. In the absence of Ca2+, Mg2+ (1 to 10 mM) did not activate the channels but modified the activating effect of Ca2+ ions: it decreased the Hill coefficient (n), reduced the apparent dissociation constant (K0.5), and modified the channel open and closed times. K0.5 was found to be a voltage-dependent parameter. In the absence of Mg2+, it averaged 600 microM at -20 mV and 27 microM at +30 mV (22 degrees C, pH 6.8). Mg2+ at saturating concentrations (5 to 10 mM) decreased K0.5 to 50 microM at -20 mV and to 15 microM at +30 mV. Irrespective of the membrane potential, K0.5 tended to its limit value of about 12.6 microM. Thus, the effects of membrane depolarization and Mg2+ exhibited a non-additive, competitive relationship. Mg2+ perturbed the exponential shape of the voltage dependences of K0.5. The Hill coefficient characterizing the interaction of Ca2+ ions with the channels was found to be voltage-dependent. In the absence of Mg2+, it increased rather sharply from approx. 2 to 3.5 when the membrane potential was raised from -10 to 0 mV. Mg2+ increased n in a dose-dependent manner; however, about a twofold increase of n occurred within a narrow concentration range (2 to 3 mM). The action of Mg2+ on n was, apparently, voltage-independent, and the effects of Mg2+ and voltage on n were seemingly additive.     

Modification of ATP-sensitive K+ channels by proteolysis in smooth muscle cells from pig urethra

Patch-clamp experiments have been performed to investigate the effects of endoproteases (such as trypsin, carboxypeptidase B) on both membrane currents and unitary currents in isolated smooth muscle cells from pig proximal urethra (conventional whole-cell configuration, cell-attached configuration, and inside-out patches). Application of either trypsin (1 mg/mL) or carboxypeptidase B (0.1 mg/mL) to the intracellular surface of the excised membrane patches stimulated the activity of a 2.1 pA K+ channel (in symmetrical 140 mM K+ conditions) at a holding potential of -50 mV. The trypsin-induced K+ channels in inside-out configuration exhibited the same amplitude and similar channel opening kinetics to the levcromakalim-induced ATP-sensitive K+ channel (i.e. K ATP channel) in cell-attached patches of the same membrane; however, the sensitivity of the channels to glibenclamide was greatly reduced after the trypsin-treatment. The activity of the trypsin-induced K+ channel was reversibly inhibited by cibenzoline in an inside-out configuration (Ki = 5 microM). It is concluded that trypsin and carboxypeptidase B reactivate the channel with an intact pore activity but the different pharmacological properties of the channels may reflect some change in the conformation in channel proteins after proteolysis.     

Potassium flux ratio in voltage-clamped squid giant axons

The potassium flux ratio across the axolemma of internally perfused, voltage-clamped giant axons of Loligo pealei has been evaluated at various membrane potentials and internal potassium concentrations ([K]i). Four different methods were used: (a) independent measurement of one-way influx and efflux of 42K; (b) simultaneous measurement of net K current (IK) and 42K influx; (c) simultaneous measurement of IK and 42K efflux; and (d) measurement of potassium conductance and 42K influx at the potassium equilibrium potential. The reliability of each of these methods is discussed. The average value of the exponent n' in the Hodgkin-Keynes equation ranged from 1.5 at -4mV and 200 mM [K]i to 3.3 at -38 mV and 350 mM [K]i and appeared to be a function of membrane potential and possibly of [K]i. It is concluded that the potassium channel of squid giant axon is a multi-ion, single-file pore with three or more sites.     

hERG K+ channel blockade by the antipsychotic drug thioridazine: An obligatory role for the S6 helix residue F656

The phenothiazine antipsychotic agent thioridazine has been linked with prolongation of the QT interval on the electrocardiogram, ventricular arrhythmias, and sudden death. Although thioridazine is known to inhibit cardiac hERG K(+) channels there is little mechanistic information on this action. We have investigated in detail hERG K(+) channel current (I(hERG)) blockade by thioridazine and identified a key molecular determinant of blockade. Whole-cell I(hERG) measurements were made at 37 degrees C from human embryonic kidney (HEK-293) cells expressing wild-type and mutant hERG channels. Thioridazine inhibited I(hERG) tails at -40mV following a 2s depolarization to +20mV with an IC(50) value of 80nM. Comparable levels of I(hERG) inhibition were seen with physiological command waveforms (ventricular and Purkinje fibre action potentials). Thioridazine block of I(hERG) was only weakly voltage-dependent, though the time dependence of I(hERG) inhibition indicated contingency of blockade upon channel gating. The S6 helix point mutation F656A almost completely abolished, and the Y652A mutation partially attenuated, I(hERG) inhibition by thioridazine. In summary, thioridazine is one of the most potent hERG K(+) channel blockers amongst antipsychotics, exhibiting characteristics of a preferential open/activated channel blocker and binding at a high affinity site in the hERG channel pore.     

External barium influences the gating charge movement of Shaker potassium channels.

External Ba2+ speeds the OFF gating currents (IgOFF) of Shaker K+ channels but only upon repolarization from potentials that are expected to open the channel pore. To study this effect we used a nonconducting and noninactivating mutant of the Shaker K+ channel, ShH4-IR (W434F). External Ba2+ slightly decreases the quantity of ON gating charge (QON) upon depolarization to potentials near -30 mV but has little effect on the quantity of charge upon stepping to more hyperpolarized or depolarized potentials. More strikingly, Ba2+ significantly increases the decay rate of IgOFF upon repolarization to -90 mV from potentials positive to approximately -55 mV. For Ba2+ to have this effect, the depolarizing command must be maintained for a duration that is dependent on the depolarizing potential (> 4 ms at -30 mV and > 1 ms at 0 mV). The actions of Ba2+ on the gating current are dose-dependent (EC50 approximately 0.2 mM) and are not produced by either Ca2+ or Mg2+ (2 mM). The results suggest that Ba2+ binds to a specific site on the Shaker K+ channel that destabilizes the open conformation and thus facilitates the return of gating charge upon repolarization.