Interaction of internal Ba2+ with a cloned Ca(2+)-dependent K+ (hslo) channel from smooth muscle

Mutation in pore-helix modulates interplay between filter gate and Ba2+ block in a Kcv channel pore

The selectivity filter of K+ channels catalyzes a rapid and highly selective transport of K+ while serving as a gate. To understand the control of this filter gate, we use the pore-only K+ channel KcvNTS in which gating is exclusively determined by the activity of the filter gate. It has been previously shown that a mutation at the C-terminus of the pore-helix (S42T) increases K+ permeability and introduces distinct voltage-dependent and K+-sensitive channel closures at depolarizing voltages. Here, we report that the latter are not generated by intrinsic conformational changes of the filter gate but by a voltage-dependent block caused by nanomolar trace contaminations of Ba2+ in the KCl solution. Channel closures can be alleviated by extreme positive voltages and they can be completely abolished by the high-affinity Ba2+ chelator 18C6TA. By contrast, the same channel closures can be augmented by adding Ba2+ at submicromolar concentrations to the cytosolic buffer. These data suggest that a conservative exchange of Ser for Thr in a crucial position of the filter gate increases the affinity of the filter for Ba2+ by >200-fold at positive voltages. While Ba2+ ions apparently remain only for a short time in the filter-binding sites of the WT channel before passing the pore, they remain much longer in the mutant channel. Our findings suggest that the dwell times of permeating and blocking ions in the filter-binding sites are tightly controlled by interactions between the pore-helix and the selectivity filter.

Methods for Investigating TRP Channel Gating

A complete characterization of temperature -and voltage-activated TRP channel gating requires a precise determination of the absolute probability of opening in a wide range of voltages, temperatures, and agonist concentrations. We have achieved this in the case of the TRPM8 channel expressed in Xenopus laevis oocytes. Measurements covered an extensive range of probabilities and unprecedented applied voltages up to 500 mV. In this chapter, we describe animal care protocols of patch-clamp pipette preparation, temperature control methods, and analysis of ionic currents to obtain reliable absolute open channel probabilities.

The first transmembrane domain (TM1) of β2-subunit binds to the transmembrane domain S1 of α-subunit in BK potassium channels

The BK channel is one of the most broadly expressed ion channels in mammals. In many tissues, the BK channel pore-forming α-subunit is associated to an auxiliary β-subunit that modulates the voltage- and Ca(2+)-dependent activation of the channel. Structural components present in β-subunits that are important for the physical association with the α-subunit are yet unknown. Here, we show through co-immunoprecipitation that the intracellular C-terminus, the second transmembrane domain (TM2) and the extracellular loop of the β2-subunit are dispensable for association with the α-subunit pointing transmembrane domain 1 (TM1) as responsible for the interaction. Indeed, the TOXCAT assay for transmembrane protein-protein interactions demonstrated for the first time that TM1 of the β2-subunit physically binds to the transmembrane S1 domain of the α-subunit.

Coupling and cooperativity in voltage activation of a limited-state BK channel gating in saturating Ca2+

Voltage-dependent gating mechanisms of large conductance Ca²⁺ and voltage-activated (BK) channels were investigated using two-dimensional maximum likelihood analysis of single-channel open and closed intervals. To obtain sufficient data at negative as well as positive voltages, single-channel currents were recorded at saturating Ca²⁺ from BK channels mutated to remove the RCK1 Ca²⁺ and Mg²⁺ sensors. The saturating Ca²⁺ acting on the Ca²⁺ bowl sensors of the resulting BK_B channels increased channel activity while driving the gating into a reduced number of states, simplifying the model. Five highly constrained idealized gating mechanisms based on extensions of the Monod-Wyman-Changeux model for allosteric proteins were examined. A 10-state model without coupling between the voltage sensors and the opening/closing transitions partially described the voltage dependence of Po but not the single-channel kinetics. With allowed coupling, the model gave improved descriptions of Po and approximated the single-channel kinetics; each activated voltage sensor increased the opening rate approximately an additional 23-fold while having little effect on the closing rate. Allowing cooperativity among voltage sensors further improved the description of the data: each activated voltage sensor increased the activation rate of the remaining voltage sensors approximately fourfold, with little effect on the deactivation rate. The coupling factor was decreased in models with cooperativity from ∼23 to ∼18. Whether the apparent cooperativity among voltage sensors arises from imposing highly idealized models or from actual cooperativity will require additional studies to resolve. For both cooperative and noncooperative models, allowing transitions to five additional brief (flicker) closed states further improved the description of the data. These observations show that the voltage-dependent single-channel kinetics of BK_B channels can be approximated by highly idealized allosteric models in which voltage sensor movement increases Po mainly through an increase in channel opening rates, with limited effects on closing rates.

Alpha5beta1 integrin engagement increases large conductance, Ca2+-activated K+ channel current and Ca2+ sensitivity through c-src-mediated channel phosphorylation

Large conductance, calcium-activated K(+) (BK) channels are important regulators of cell excitability and recognized targets of intracellular kinases. BK channel modulation by tyrosine kinases, including focal adhesion kinase and c-src, suggests their potential involvement in integrin signaling. Recently, we found that fibronectin, an endogenous alpha5beta1 integrin ligand, enhances BK channel current through both Ca(2+)- and phosphorylation-dependent mechanisms in vascular smooth muscle. Here, we show that macroscopic currents from HEK 293 cells expressing murine BK channel alpha-subunits (mSlo) are acutely potentiated following alpha5beta1 integrin activation. The effect occurs in a Ca(2+)-dependent manner, 1-3 min after integrin engagement. After integrin activation, normalized conductance-voltage relations for mSlo are left-shifted at free Ca(2+) concentrations >or=1 microm. Overexpression of human c-src with mSlo, in the absence of integrin activation, leads to similar shifts in mSlo Ca(2+) sensitivity, whereas overexpression of catalytically inactive c-src blocks integrin-induced potentiation. However, neither integrin activation nor c-src overexpression potentiates current in BK channels containing a point mutation at Tyr-766. Biochemical tests confirmed the critical importance of residue Tyr-766 in integrin-induced channel phosphorylation. Thus, BK channel activity is enhanced by alpha5beta1 integrin activation, likely through an intracellular signaling pathway involving c-src phosphorylation of the channel alpha-subunit at Tyr-766. The net result is increased current amplitude, enhanced Ca(2+) sensitivity, and rate of activation of the BK channel, which would collectively promote smooth muscle hyperpolarization in response to integrin-extracellular matrix interactions.

An extracellular Cu2+ binding site in the voltage sensor of BK and Shaker potassium channels

Copper is an essential trace element that may serve as a signaling molecule in the nervous system. Here we show that extracellular Cu²⁺ is a potent inhibitor of BK and Shaker K⁺ channels. At low micromolar concentrations, Cu²⁺ rapidly and reversibly reduces macrosocopic K⁺ conductance (G_K) evoked from mSlo1 BK channels by membrane depolarization. G_K is reduced in a dose-dependent manner with an IC₅₀ and Hill coefficient of ∼2 μM and 1.0, respectively. Saturating 100 μM Cu²⁺ shifts the G_K-V relation by +74 mV and reduces G_Kmax by 27% without affecting single channel conductance. However, 100 μM Cu²⁺ fails to inhibit G_K when applied during membrane depolarization, suggesting that Cu²⁺ interacts poorly with the activated channel. Of other transition metal ions tested, only Zn²⁺ and Cd²⁺ had significant effects at 100 μM with IC₅₀s > 0.5 mM, suggesting the binding site is Cu²⁺ selective. Mutation of external Cys or His residues did not alter Cu²⁺ sensitivity. However, four putative Cu²⁺-coordinating residues were identified (D133, Q151, D153, and R207) in transmembrane segments S1, S2, and S4 of the mSlo1 voltage sensor, based on the ability of substitutions at these positions to alter Cu²⁺ and/or Cd²⁺ sensitivity. Consistent with the presence of acidic residues in the binding site, Cu²⁺ sensitivity was reduced at low extracellular pH. The three charged positions in S1, S2, and S4 are highly conserved among voltage-gated channels and could play a general role in metal sensitivity. We demonstrate that Shaker, like mSlo1, is much more sensitive to Cu²⁺ than Zn²⁺ and that sensitivity to these metals is altered by mutating the conserved positions in S1 or S4 or reducing pH. Our results suggest that the voltage sensor forms a state- and pH-dependent, metal-selective binding pocket that may be occupied by Cu²⁺ at physiologically relevant concentrations to inhibit activation of BK and other channels.

Intrinsic electrostatic potential in the BK channel pore: role in determining single channel conductance and block

The internal vestibule of large-conductance Ca²⁺ voltage-activated K⁺ (BK) channels contains a ring of eight negative charges not present in K⁺ channels of lower conductance (Glu386 and Glu389 in hSlo) that modulates channel conductance through an electrostatic mechanism (Brelidze, T.I., X. Niu, and K.L. Magleby. 2003. Proc. Natl. Acad. Sci. USA. 100:9017–9022). In BK channels there are also two acidic amino acid residues in an extracellular loop (Asp326 and Glu329 in hSlo). To determine the electrostatic influence of these charges on channel conductance, we expressed wild-type BK channels and mutants E386N/E389N, D326N, E329Q, and D326N/E329Q channels on Xenopus laevis oocytes, and measured the expressed currents under patch clamp. Contribution of E329 to the conductance is negligible and single channel conductance of D326N/E329Q channels measured at 0 mV in symmetrical 110 mM K⁺ was 18% lower than the control. Current–voltage curves displayed weak outward rectification for D326N and the double mutant. The conductance differences between the mutants and wild-type BK were caused by an electrostatic effect since they were enhanced at low K⁺ (30 mM) and vanished at high K⁺ (1 M K⁺). We determine the electrostatic potential change, Δφ, caused by the charge neutralization using TEA⁺ block for the extracellular charges and Ba²⁺ for intracellular charges. We measured 13 ± 2 mV for Δφ at the TEA⁺ site when turning off the extracellular charges, and 17 ± 2 mV for the Δφ at the Ba²⁺ site when the intracellular charges were turned off. To understand the electrostatic effect of charge neutralizations, we determined Δφ using a BK channel molecular model embedded in a lipid bilayer and solving the Poisson-Boltzmann equation. The model explains the experimental results adequately and, in particular, gives an economical explanation to the differential effect on the conductance of the neutralization of charges D326 and E329.

Mg2+ enhances voltage sensor/gate coupling in BK channels

BK (Slo1) potassium channels are activated by millimolar intracellular Mg²⁺ as well as micromolar Ca²⁺ and membrane depolarization. Mg²⁺ and Ca²⁺ act in an approximately additive manner at different binding sites to shift the conductance–voltage (G_K-V) relation, suggesting that these ligands might work through functionally similar but independent mechanisms. However, we find that the mechanism of Mg²⁺ action is highly dependent on voltage sensor activation and therefore differs fundamentally from that of Ca²⁺. Evidence that Ca²⁺ acts independently of voltage sensor activation includes an ability to increase open probability (P_O) at extreme negative voltages where voltage sensors are in the resting state; 2 μM Ca²⁺ increases P_O more than 15-fold at −120 mV. However 10 mM Mg²⁺, which has an effect on the G_K-V relation similar to 2 μM Ca²⁺, has no detectable effect on P_O when voltage sensors are in the resting state. Gating currents are only slightly altered by Mg²⁺ when channels are closed, indicating that Mg²⁺ does not act merely to promote voltage sensor activation. Indeed, channel opening is facilitated in a voltage-independent manner by Mg²⁺ in a mutant (R210C) whose voltage sensors are constitutively activated. Thus, 10 mM Mg²⁺ increases P_O only when voltage sensors are activated, effectively strengthening the allosteric coupling of voltage sensor activation to channel opening. Increasing Mg²⁺ from 10 to 100 mM, to occupy very low affinity binding sites, has additional effects on gating that more closely resemble those of Ca²⁺. The effects of Mg²⁺ on steady-state activation and I_K kinetics are discussed in terms of an allosteric gating scheme and the state-dependent interactions between Mg²⁺ and voltage sensor that may underlie this mechanism.

State-dependent block of BK channels by synthesized shaker ball peptides

Crystal structures of potassium channels have strongly corroborated an earlier hypothetical picture based on functional studies, in which the channel gate was located on the cytoplasmic side of the pore. However, accessibility studies on several types of ligand-sensitive K⁺ channels have suggested that their activation gates may be located near or within the selectivity filter instead. It remains to be determined to what extent the physical location of the gate is conserved across the large K⁺ channel family. Direct evidence about the location of the gate in large conductance calcium-activated K⁺ (BK) channels, which are gated by both voltage and ligand (calcium), has been scarce. Our earlier kinetic measurements of the block of BK channels by internal quaternary ammonium ions have raised the possibility that they may lack a cytoplasmic gate. We show in this study that a synthesized Shaker ball peptide (ShBP) homologue acts as a state-dependent blocker for BK channels when applied internally, suggesting a widening at the intracellular end of the channel pore upon gating. This is consistent with a gating-related conformational change at the cytoplasmic end of the pore-lining helices, as suggested by previous functional and structural studies on other K⁺ channels. Furthermore, our results from two BK channel mutations demonstrate that similar types of interactions between ball peptides and channels are shared by BK and other K⁺ channel types.

Role of charged residues in the S1-S4 voltage sensor of BK channels

The activation of large conductance Ca²⁺-activated (BK) potassium channels is weakly voltage dependent compared to Shaker and other voltage-gated K⁺ (K_V) channels. Yet BK and K_V channels share many conserved charged residues in transmembrane segments S1–S4. We mutated these residues individually in mSlo1 BK channels to determine their role in voltage gating, and characterized the voltage dependence of steady-state activation (P_o) and I_K kinetics (τ(I_K)) over an extended voltage range in 0–50 μM [Ca²⁺]_i. mSlo1 contains several positively charged arginines in S4, but only one (R213) together with residues in S2 (D153, R167) and S3 (D186) are potentially voltage sensing based on the ability of charge-altering mutations to reduce the maximal voltage dependence of P_O. The voltage dependence of P_O and τ(I_K) at extreme negative potentials was also reduced, implying that the closed–open conformational change and voltage sensor activation share a common source of gating charge. Although the position of charged residues in the BK and K_V channel sequence appears conserved, the distribution of voltage-sensing residues is not. Thus the weak voltage dependence of BK channel activation does not merely reflect a lack of charge but likely differences with respect to K_V channels in the position and movement of charged residues within the electric field. Although mutation of most sites in S1–S4 did not reduce gating charge, they often altered the equilibrium constant for voltage sensor activation. In particular, neutralization of R207 or R210 in S4 stabilizes the activated state by 3–7 kcal mol⁻¹, indicating a strong contribution of non–voltage-sensing residues to channel function, consistent with their participation in state-dependent salt bridge interactions. Mutations in S4 and S3 (R210E, D186A, and E180A) also unexpectedly weakened the allosteric coupling of voltage sensor activation to channel opening. The implications of our findings for BK channel voltage gating and general mechanisms of voltage sensor activation are discussed.

Generation of functional fluorescent BK channels by random insertion of GFP variants

The yellow and cyan variants of green fluorescent protein (GFP) constitute an excellent pair for fluorescence resonance energy transfer (FRET) and can be used to study conformational rearrangements of proteins. Our aim was to develop a library of fluorescent large conductance voltage- and Ca2+-gated channels (BK or slo channels) for future use in FRET studies. We report the results of a random insertion of YFP and CFP into multiple sites of the alpha subunit of the hslo channel using a Tn5 transposon-based technique. 55 unique fluorescent fusion proteins were obtained and tested for cell surface expression and channel function. 19 constructs are expressed at the plasma membrane and show voltage and Ca2+-dependent currents. In 16 of them the voltage and Ca2+ dependence is very similar to the wild-type channel. Two insertions in the Ca2+ bowl and one in the RCK2 domain showed a strong shift in the G-V curve. The remaining 36 constructs were retained intracellularly; a solubility assay suggests that these proteins are not forming intracellular aggregates. The "success rate" of 19 out of 55 hslo insertion constructs compares very favorably with other studies of random GFP fusions.

Cysteine modification alters voltage- and Ca(2+)-dependent gating of large conductance (BK) potassium channels

The Ca²⁺-activated K⁺ (BK) channel α-subunit contains many cysteine residues within its large COOH-terminal tail domain. To probe the function of this domain, we examined effects of cysteine-modifying reagents on channel gating. Application of MTSET, MTSES, or NEM to mSlo1 or hSlo1 channels changed the voltage and Ca²⁺ dependence of steady-state activation. These reagents appear to modify the same cysteines but have different effects on function. MTSET increases I_K and shifts the G_K–V relation to more negative voltages, whereas MTSES and NEM shift the G_K–V in the opposite direction. Steady-state activation was altered in the presence or absence of Ca²⁺ and at negative potentials where voltage sensors are not activated. Combinations of [Ca²⁺] and voltage were also identified where P_o is not changed by cysteine modification. Interpretation of our results in terms of an allosteric model indicate that cysteine modification alters Ca²⁺ binding and the relative stability of closed and open conformations as well as the coupling of voltage sensor activation and Ca²⁺ binding and to channel opening. To identify modification-sensitive residues, we examined effects of MTS reagents on mutant channels lacking one or more cysteines. Surprisingly, the effects of MTSES on both voltage- and Ca²⁺-dependent gating were abolished by replacing a single cysteine (C430) with alanine. C430 lies in the RCK1 (regulator of K⁺ conductance) domain within a series of eight residues that is unique to BK channels. Deletion of these residues shifted the G_K–V relation by >−80 mV. Thus we have identified a region that appears to strongly influence RCK domain function, but is absent from RCK domains of known structure. C430A did not eliminate effects of MTSET on apparent Ca²⁺ affinity. However an additional mutation, C615S, in the Haem binding site reduced the effects of MTSET, consistent with a role for this region in Ca²⁺ binding.

Regulation of K+ flow by a ring of negative charges in the outer pore of BKCa channels. Part II: Neutralization of aspartate 292 reduces long channel openings and gating current slow component

Neutralization of the aspartate near the selectivity filter in the GYGD pore sequence (D292N) of the voltage- and Ca²⁺-activated K⁺ channel (MaxiK, BKCa) does not prevent conduction like the corresponding mutation in Shaker channel, but profoundly affects major biophysical properties of the channel (Haug, T., D. Sigg, S. Ciani, L. Toro, E. Stefani, and R. Olcese. 2004. J. Gen. Physiol. 124:173–184). Upon depolarizations, the D292N mutant elicited mostly gating current, followed by small or no ionic current, at voltages where the wild-type hSlo channel displayed robust ionic current. In fact, while the voltage dependence of the gating current was not significantly affected by the mutation, the overall activation curve was shifted by ∼20 mV toward more depolarized potentials. Several lines of evidence suggest that the mutation prevents population of certain open states that in the wild type lead to high open probability. The activation curves of WT and D292N can both be fitted to the sum of two Boltzmann distributions with identical slope factors and half activation potentials, just by changing their relative amplitudes. The steeper and more negative component of the activation curve was drastically reduced by the D292N mutation (from 0.65 to 0.30), suggesting that the population of open states that occurs early in the activation pathway is reduced. Furthermore, the slow component of the gating current, which has been suggested to reflect transitions from closed to open states, was greatly reduced in D292N channels. The D292N mutation also affected the limiting open probability: at 0 mV, the limiting open probability dropped from ∼0.5 for the wild-type channel to 0.06 in D292N (in 1 mM [Ca²⁺]_i). In addition to these effects on gating charge and open probability, as already described in Part I, the D292N mutation introduces a ∼40% reduction of outward single channel conductance, as well as a strong outward rectification.

Mapping the BKCa channel's "Ca2+ bowl": side-chains essential for Ca2+ sensing

There is controversy over whether Ca²⁺ binds to the BK_Ca channel's intracellular domain or its integral-membrane domain and over whether or not mutations that reduce the channel's Ca²⁺ sensitivity act at the point of Ca²⁺ coordination. One region in the intracellular domain that has been implicated in Ca²⁺ sensing is the “Ca²⁺ bowl”. This region contains many acidic residues, and large Ca²⁺-bowl mutations eliminate Ca²⁺ sensing through what appears to be one type of high-affinity Ca²⁺-binding site. Here, through site-directed mutagenesis we have mapped the residues in the Ca²⁺ bowl that are most important for Ca²⁺ sensing. We find acidic residues, D898 and D900, to be essential, and we find them essential as well for Ca²⁺ binding to a fusion protein that contains a portion of the BK_Ca channel's intracellular domain. Thus, much of our data supports the conclusion that Ca²⁺ binds to the BK_Ca channel's intracellular domain, and they define the Ca²⁺ bowl's essential Ca²⁺-sensing motif. Overall, however, we have found that the relationship between mutations that disrupt Ca²⁺ sensing and those that disrupt Ca²⁺ binding is not as strong as we had expected, a result that raises the possibility that, when examined by gel-overlay, the Ca²⁺ bowl may be in a nonnative conformation.

Protons block BK channels by competitive inhibition with K+ and contribute to the limits of unitary currents at high voltages

Proton block of unitary currents through BK channels was investigated with single-channel recording. Increasing intracellular proton concentration decreased unitary current amplitudes with an apparent pKa of 5.1 without discrete blocking events, indicating fast proton block. Unitary currents recorded at pH_i 8.0 and 9.0 had the same amplitudes, indicating that 10⁻⁸ M H⁺ had little blocking effect. Increasing H⁺ by recording at pH_i 7.0, 6.0, and 5.0 then reduced the unitary currents by 13%, 25%, and 53%, respectively, at +200 mV. Increasing K⁺_i relieved the proton block in a manner consistent with competitive inhibition of K⁺_i action by H⁺_i. Proton block was voltage dependent, increasing with depolarization, indicating that block was coupled to the electric field of the membrane. Proton block was not described by the Woodhull equation for noncompetitive voltage-dependent block, but was described by an equation for cooperative competitive inhibition that included voltage-dependent block from the Woodhull equation. Proton block was still present after replacing the eight negative charges in the ring of charge at the entrance to the intracellular vestibule by uncharged amino acids. Thus, the ring of charge is not the site of proton block or of competitive inhibition of K⁺_i action by H⁺_i. With 150 mM symmetrical KCl, unitary current amplitudes increased with depolarization, reaching 66 pA at +350 mV (pH_i 7.0). The increase in amplitude with voltage became sublinear for voltages >100 mV. The sublinearity was unaffected by removing from the intracellular solutions Ca²⁺ and Ba²⁺ ions, the Ca²⁺ buffers EGTA and HEDTA, the pH buffer TES, or by replacing Cl⁻ with MeSO₃⁻. Proton block accounted for ∼40% of the sublinearity at +200 mV and pH 7.0, indicating that factors in addition to proton block contribute to the sublinearity of the unitary currents through BK channels.

Unique inner pore properties of BK channels revealed by quaternary ammonium block

Potassium channels have a very wide distribution of single-channel conductance, with BK type Ca²⁺-activated K⁺ channels having by far the largest. Even though crystallographic views of K⁺ channel pores have become available, the structural basis underlying BK channels' large conductance has not been completely understood. In this study we use intracellularly applied quaternary ammonium compounds to probe the pore of BK channels. We show that molecules as large as decyltriethylammonium (C₁₀) and tetrabutylammonium (TBA) have much faster block and unblock rates in BK channels when compared with any other tested K⁺ channel types. Additionally, our results suggest that at repolarization large QA molecules may be trapped inside blocked BK channels without slowing the overall process of deactivation. Based on these findings we propose that BK channels may differ from other K⁺ channels in its geometrical design at the inner mouth, with an enlarged cavity and inner pore providing less spatially restricted access to the cytoplasmic solution. These features could potentially contribute to the large conductance of BK channels.

A ring of eight conserved negatively charged amino acids doubles the conductance of BK channels and prevents inward rectification

Large-conductance Ca2+-voltage-activated K+ channels (BK channels) control many key physiological processes, such as neurotransmitter release and muscle contraction. A signature feature of BK channels is that they have the largest single channel conductance of all K+ channels. Here we examine the mechanism of this large conductance. Comparison of the sequence of BK channels to lower-conductance K+ channels and to a crystallized bacterial K+ channel (MthK) revealed that BK channels have a ring of eight negatively charged glutamate residues at the entrance to the intracellular vestibule. This ring of charge, which is absent in lower-conductance K+ channels, is shown to double the conductance of BK channels for outward currents by increasing the concentration of K+ in the vestibule through an electrostatic mechanism. Removing the ring of charge converts BK channels to inwardly rectifying channels. Thus, a simple electrostatic mechanism contributes to the large conductance of BK channels.

Coupling between voltage sensor activation, Ca2+ binding and channel opening in large conductance (BK) potassium channels

To determine how intracellular Ca(2+) and membrane voltage regulate the gating of large conductance Ca(2+)-activated K(+) (BK) channels, we examined the steady-state and kinetic properties of mSlo1 ionic and gating currents in the presence and absence of Ca(2+) over a wide range of voltage. The activation of unliganded mSlo1 channels can be accounted for by allosteric coupling between voltage sensor activation and the closed (C) to open (O) conformational change (Horrigan, F.T., and R.W. Aldrich. 1999. J. Gen. Physiol. 114:305-336; Horrigan, F.T., J. Cui, and R.W. Aldrich. 1999. J. Gen. Physiol. 114:277-304). In 0 Ca(2+), the steady-state gating charge-voltage (Q(SS)-V) relationship is shallower and shifted to more negative voltages than the conductance-voltage (G(K)-V) relationship. Calcium alters the relationship between Q-V and G-V, shifting both to more negative voltages such that they almost superimpose in 70 microM Ca(2+). This change reflects a differential effect of Ca(2+) on voltage sensor activation and channel opening. Ca(2+) has only a small effect on the fast component of ON gating current, indicating that Ca(2+) binding has little effect on voltage sensor activation when channels are closed. In contrast, open probability measured at very negative voltages (less than -80 mV) increases more than 1,000-fold in 70 microM Ca(2+), demonstrating that Ca(2+) increases the C-O equilibrium constant under conditions where voltage sensors are not activated. Thus, Ca(2+) binding and voltage sensor activation act almost independently, to enhance channel opening. This dual-allosteric mechanism can reproduce the steady-state behavior of mSlo1 over a wide range of conditions, with the assumption that activation of individual Ca(2+) sensors or voltage sensors additively affect the energy of the C-O transition and that a weak interaction between Ca(2+) sensors and voltage sensors occurs independent of channel opening. By contrast, macroscopic I(K) kinetics indicate that Ca(2+) and voltage dependencies of C-O transition rates are complex, leading us to propose that the C-O conformational change may be described by a complex energy landscape.

Elimination of the BK(Ca) channel's high-affinity Ca(2+) sensitivity

We report here a combination of site-directed mutations that eliminate the high-affinity Ca(2+) response of the large-conductance Ca(2+)-activated K(+) channel (BK(Ca)), leaving only a low-affinity response blocked by high concentrations of Mg(2+). Mutations at two sites are required, the "Ca(2+) bowl," which has been implicated previously in Ca(2+) binding, and M513, at the end of the channel's seventh hydrophobic segment. Energetic analyses of mutations at these positions, alone and in combination, argue that the BK(Ca) channel contains three types of Ca(2+) binding sites, one of low affinity that is Mg(2+) sensitive (as has been suggested previously) and two of higher affinity that have similar binding characteristics and contribute approximately equally to the power of Ca(2+) to influence channel opening. Estimates of the binding characteristics of the BK(Ca) channel's high-affinity Ca(2+)-binding sites are provided.

Specific localization of an inwardly rectifying K(+) channel, Kir4.1, at the apical membrane of rat gastric parietal cells; its possible involvement in K(+) recycling for the H(+)-K(+)-pump

Hydrochloric acid (HCl) is produced in parietal cells of gastric epithelium by a H(+)-K(+) pump. Protons are secreted into the gastric lumen in exchange for K(+) by the action of the H(+)-K(+)-ATPase. Luminal K(+) is essential for the operation of the pump and is thought to be supplied by unidentified K(+) channels localized at the apical membrane of parietal cells. In this study, we showed that histamine- and carbachol-induced acid secretion from isolated parietal cells monitored by intracellular accumulation of aminopyrine was depressed by Ba(2+), an inhibitor of inwardly rectifying K(+) channels. Among members of the inwardly rectifying K(+) channel family, we found with reverse transcriptase-polymerase chain reaction analyses that Kir4.1, Kir4.2 and Kir7.1 were expressed in rat gastric mucosa. With immunohistochemical analyses, Kir4.1 was found to be expressed in gastric parietal cells and localized specifically at their apical membrane. The current flowing through Kir4.1 channel expressed in HEK293T cells was not affected by reduction of extracellular pH from 7.4 to 3. These results suggest that Kir4.1 may be involved in the K(+) recycling pathway in the apical membrane which is required for activation of the H(+)-K(+) pump in gastric parietal cells.

Ca(2+)-activated K+ channel inhibition by reactive oxygen species

We studied the effect of H(2)O(2) on the gating behavior of large-conductance Ca(2+)-sensitive voltage-dependent K(+) (K(V,Ca)) channels. We recorded potassium currents from single skeletal muscle channels incorporated into bilayers or using macropatches of Xenopus laevis oocytes membranes expressing the human Slowpoke (hSlo) alpha-subunit. Exposure of the intracellular side of K(V,Ca) channels to H(2)O(2) (4-23 mM) leads to a time-dependent decrease of the open probability (P(o)) without affecting the unitary conductance. H(2)O(2) did not affect channel activity when added to the extracellular side. These results provide evidence for an intracellular site(s) of H(2)O(2) action. Desferrioxamine (60 microM) and cysteine (1 mM) completely inhibited the effect of H(2)O(2), indicating that the decrease in P(o) was mediated by hydroxyl radicals. The reducing agent dithiothreitol (DTT) could not fully reverse the effect of H(2)O(2). However, DTT did completely reverse the decrease in P(o) induced by the oxidizing agent 5,5'-dithio-bis-(2-nitrobenzoic acid). The incomplete recovery of K(V,Ca) channel activity promoted by DTT suggests that H(2)O(2) treatment must be modifying other amino acid residues, e.g., as methionine or tryptophan, besides cysteine. Noise analysis of macroscopic currents in Xenopus oocytes expressing hSlo channels showed that H(2)O(2) induced a decrease in current mediated by a decrease both in the number of active channels and P(o).

Allosteric linkage between voltage and Ca(2+)-dependent activation of BK-type mslo1 K(+) channels

The activation of BK type Ca(2+)-activated K(+) channels depends on both voltage and Ca(2+). We studied three point mutations in the putative voltage sensor S4 or S4-S5 linker regions in the mslo1 BK channels to explore the relationship between voltage and Ca(2+) in activating the channel. These mutations reduced the steepness of the open probability - voltage (P(o) - V) relation and increased the shift of the P(o) - V relations on the voltage axis in response to increases in the calcium concentration. It is striking that these two effects were reciprocally related for all three mutations, despite different effects of the mutations on other aspects of the voltage dependence of channel gating. This reciprocal relationship suggests strongly that the free energy contributions to channel activation provided by voltage and by calcium binding are simply additive. We conclude that the Ca(2+) binding sites and the voltage sensors do not directly interact. Rather they both affect the mslo1 channel opening through an allosteric mechanism, by influencing the conformational change between the closed and open conformations. The mutations changed the channel's voltage dependence with little effect on its Ca(2+) affinitiy.

Role of the beta1 subunit in large-conductance Ca(2+)-activated K(+) channel gating energetics. Mechanisms of enhanced Ca(2+) sensitivity

Over the past few years, it has become clear that an important mechanism by which large-conductance Ca(2+)-activated K(+) channel (BK(Ca)) activity is regulated is the tissue-specific expression of auxiliary beta subunits. The first of these to be identified, beta1, is expressed predominately in smooth muscle and causes dramatic effects, increasing the apparent affinity of the channel for Ca(2+) 10-fold at 0 mV, and shifting the range of voltages over which the channel activates -80 mV at 9.1 microM Ca(2+). With this study, we address the question: which aspects of BK(Ca) gating are altered by beta1 to bring about these effects: Ca(2+) binding, voltage sensing, or the intrinsic energetics of channel opening? The approach we have taken is to express the beta1 subunit together with the BK(Ca) alpha subunit in Xenopus oocytes, and then to compare beta1's steady state effects over a wide range of Ca(2+) concentrations and membrane voltages to those predicted by allosteric models whose parameters have been altered to mimic changes in the aspects of gating listed above. The results of our analysis suggest that much of beta1's steady state effects can be accounted for by a reduction in the intrinsic energy the channel must overcome to open and a decrease in its voltage sensitivity, with little change in the affinity of the channel for Ca(2+) when it is either open or closed. Interestingly, however, the small changes in Ca(2+) binding affinity suggested by our analysis (K(c) 7.4 microM --> 9.6 microM; K(o) = 0.80 microM --> 0.65 microM) do appear to be functionally important. We also show that beta1 affects the mSlo conductance-voltage relation in the essential absence of Ca(2+), shifting it +20 mV and reducing its apparent gating charge 38%, and we develop methods for distinguishing between alterations in Ca(2+) binding and other aspects of BK(Ca) channel gating that may be of general use.

Complex voltage-dependent behavior of single unliganded calcium-sensitive potassium channels

study and characterization of unliganded openings is of central significance for the elucidation of gating mechanisms for allosteric ligand-gated ion channels. Unliganded openings have been reported for many channel types, but their low open probability can make it difficult to study their kinetics in detail. Because the large conductance calcium-activated potassium channel mSlo is sensitive to both intracellular calcium and to membrane potential, we have been able to obtain stable unliganded single-channel recordings of mSlo with relatively high opening probability. We have found that the single-channel gating behavior of mSlo is complex, with multiple open and closed states, even when no ligand is present. Our results rule out a Monod-Wyman-Changeux allosteric mechanism with a central voltage-dependent concerted step, and they support the existence of quaternary states with less than the full number of voltage sensors activated, as has been suggested by previous work involving measurements of gating currents.

Localization of the K+ lock-In and the Ba2+ binding sites in a voltage-gated calcium-modulated channel. Implications for survival of K+ permeability

Using Ba2+ as a probe, we performed a detailed characterization of an external K+ binding site located in the pore of a large conductance Ca2+-activated K+ (BKCa) channel from skeletal muscle incorporated into planar lipid bilayers. Internal Ba2+ blocks BKCa channels and decreasing external K+ using a K+ chelator, (+)-18-Crown-6-tetracarboxylic acid, dramatically reduces the duration of the Ba2+-blocked events. Average Ba2+ dwell time changes from 10 s at 10 mM external K+ to 100 ms in the limit of very low [K+]. Using a model where external K+ binds to a site hindering the exit of Ba2+ toward the external side (Neyton, J., and C. Miller. 1988. J. Gen. Physiol. 92:549-568), we calculated a dissociation constant of 2.7 mircoM for K) at this lock-in site. We also found that BK(Ca) channels enter into a long-lasting nonconductive state when the external [K+] is reduced below 4 microM using the crown ether. Channel activity can be recovered by adding K+, Rb+, Cs+, or NH4+ to the external solution. These results suggest that the BK(Ca) channel stability in solutions of very low [K+] is due to K+ binding to a site having a very high affinity. Occupancy of this site by K+ avoids the channel conductance collapse and the exit of Ba2+ toward the external side. External tetraethylammonium also reduced the Ba2+ off rate and impeded the channel from entering into the long-lasting nonconductive state. This effect requires the presence of external K+. It is explained in terms of a model in which the conduction pore contains Ba2+, K+, and tetraethylammonium simultaneously, with the K+ binding site located internal to the tetraethylammonium site. Altogether, these results and the known potassium channel structure (Doyle, D.A., J.M. Cabral, R.A. Pfuetzner, A. Kuo, J.M. Gulbis, S.L. Cohen, B.T. Chait, and R. MacKinnon. 1998. Science. 280:69-77) imply that the lock-in site and the Ba2+ sites are the external and internal ion sites of the selectivity filter, respectively.

Allosteric voltage gating of potassium channels II. Mslo channel gating charge movement in the absence of Ca(2+)

Large-conductance Ca(2+)-activated K(+) channels can be activated by membrane voltage in the absence of Ca(2+) binding, indicating that these channels contain an intrinsic voltage sensor. The properties of this voltage sensor and its relationship to channel activation were examined by studying gating charge movement from mSlo Ca(2+)-activated K(+) channels in the virtual absence of Ca(2+) (<1 nM). Charge movement was measured in response to voltage steps or sinusoidal voltage commands. The charge-voltage relationship (Q-V) is shallower and shifted to more negative voltages than the voltage-dependent open probability (G-V). Both ON and OFF gating currents evoked by brief (0.5-ms) voltage pulses appear to decay rapidly (tau(ON) = 60 microseconds at +200 mV, tau(OFF) = 16 microseconds at -80 mV). However, Q(OFF) increases slowly with pulse duration, indicating that a large fraction of ON charge develops with a time course comparable to that of I(K) activation. The slow onset of this gating charge prevents its detection as a component of I(gON), although it represents approximately 40% of the total charge moved at +140 mV. The decay of I(gOFF) is slowed after depolarizations that open mSlo channels. Yet, the majority of open channel charge relaxation is too rapid to be limited by channel closing. These results can be understood in terms of the allosteric voltage-gating scheme developed in the preceding paper (Horrigan, F.T., J. Cui, and R.W. Aldrich. 1999. J. Gen. Physiol. 114:277-304). The model contains five open (O) and five closed (C) states arranged in parallel, and the kinetic and steady-state properties of mSlo gating currents exhibit multiple components associated with C-C, O-O, and C-O transitions.

Allosteric voltage gating of potassium channels I. Mslo ionic currents in the absence of Ca(2+)

Activation of large conductance Ca(2+)-activated K(+) channels is controlled by both cytoplasmic Ca(2+) and membrane potential. To study the mechanism of voltage-dependent gating, we examined mSlo Ca(2+)-activated K(+) currents in excised macropatches from Xenopus oocytes in the virtual absence of Ca(2+) (<1 nM). In response to a voltage step, I(K) activates with an exponential time course, following a brief delay. The delay suggests that rapid transitions precede channel opening. The later exponential time course suggests that activation also involves a slower rate-limiting step. However, the time constant of I(K) relaxation [tau(I(K))] exhibits a complex voltage dependence that is inconsistent with models that contain a single rate limiting step. tau(I(K)) increases weakly with voltage from -500 to -20 mV, with an equivalent charge (z) of only 0.14 e, and displays a stronger voltage dependence from +30 to +140 mV (z = 0.49 e), which then decreases from +180 to +240 mV (z = -0.29 e). Similarly, the steady state G(K)-V relationship exhibits a maximum voltage dependence (z = 2 e) from 0 to +100 mV, and is weakly voltage dependent (z congruent with 0.4 e) at more negative voltages, where P(o) = 10(-5)-10(-6). These results can be understood in terms of a gating scheme where a central transition between a closed and an open conformation is allosterically regulated by the state of four independent and identical voltage sensors. In the absence of Ca(2+), this allosteric mechanism results in a gating scheme with five closed (C) and five open (O) states, where the majority of the channel's voltage dependence results from rapid C-C and O-O transitions, whereas the C-O transitions are rate limiting and weakly voltage dependent. These conclusions not only provide a framework for interpreting studies of large conductance Ca(2+)-activated K(+) channel voltage gating, but also have important implications for understanding the mechanism of Ca(2+) sensitivity.

Structural determinants of gating in inward-rectifier K+ channels

The gating characteristics of two ion channels in the inward-rectifier K+ channel superfamily were compared at the single-channel level. The strong inward rectifier IRK1 (Kir 2.1) opened and closed with kinetics that were slow relative to those of the weakly rectifying ROMK2 (Kir 1.1b). At a membrane potential of -60 mV, both IRK and ROMK had single-exponential open-time distributions, with mean open times of 279 +/- 58 ms (n = 4) for IRK1 and 23 +/- 1 ms (n = 7) for ROMK. At -60 mV (and no EDTA) ROMK2 had two closed times: 1.3 +/- 0.1 and 36 +/- 3 ms (n = 7). Under the same conditions, IRK1 exhibited four discrete closed states with mean closed times of 0.8 +/- 0.1 ms, 14 +/- 0.6 ms, 99 +/- 19 ms, and 2744 +/- 640 ms (n = 4). Both the open and the three shortest closed-time constants of IRK1 decreased monotonically with membrane hyperpolarization. IRK1 open probability (Po) decreased sharply with hyperpolarization due to an increase in the frequency of long closed events that were attributable to divalent-cation blockade. Chelation of divalent cations with EDTA eliminated the slowest closed-time distribution of IRK1 and blunted the hyperpolarization-dependent fall in open probability. In contrast, ROMK2 had shorter open and closed times and only two closed states, and its Po was less affected by hyperpolarization. Chimeric channels were constructed to address the question of which parts of the molecules were responsible for the differences in kinetics. The property of multiple closed states was conferred by the second membrane-spanning domain (M2) of IRK. The long-lived open and closed states, including the higher sensitivity to extracellular divalent cations, correlated with the extracellular loop of IRK, including the "P-region." Channel kinetics were essentially unaffected by the N- and C-termini. The data of the present study are consistent with the idea that the locus of gating is near the outer mouth of the pore.

Permeation and gating of an inwardly rectifying potassium channel. Evidence for a variable energy well

Permeation, gating, and their interrelationship in an inwardly rectifying potassium (K+) channel, ROMK2, were studied using heterologous expression in Xenopus oocytes. Patch-clamp recordings of single channels were obtained in the cell-attached mode. The gating kinetics of ROMK2 were well described by a model having one open and two closed states. One closed state was short lived (approximately 1 ms) and the other was longer lived (approximately 40 ms) and less frequent (approximately 1%). The long closed state was abolished by EDTA, suggesting that it was due to block by divalent cations. These closures exhibit a biphasic voltage dependence, implying that the divalent blockers can permeate the channel. The short closures had a similar biphasic voltage dependence, suggesting that they could be due to block by monovalent, permeating cations. The rate of entering the short closed state varied with the K+ concentration and was proportional to current amplitude, suggesting that permeating K+ ions may be related to the short closures. To explain the results, we propose a variable intrapore energy well model in which a shallow well may change into a deep one, resulting in a normally permeant K+ ion becoming a blocker of its own channel.

Ca2+-dependent inactivation of large conductance Ca2+-activated K+ (BK) channels in rat hippocampal neurones produced by pore block from an associated particle

1. Recordings of the activity of the large conductance Ca2+-activated K+ (BK) channel from over 90 % of inside-out patches excised from acutely dissociated hippocampal CA1 neurones revealed an inactivation process dependent upon the presence of at least 1 microM intracellular Ca2+. Inactivation was characterized by a sudden switch from sustained high open probability (Po) long open time behaviour to extremely low Po, short open time channel activity. The low Po state (mean Po, 0.001) consisted of very short openings (time constant (tau), approximately 0.14 ms) and rare longer duration openings (tau, approximately 3.0 ms). 2. Channel inactivation occurred with a highly variable time course being observed either prior to or immediately upon patch excision, or after up to 2 min of inside-out recording. Inactivation persisted whilst recording conditions were constant. 3. Inactivation was reversed by membrane hyperpolarization, the rate of recovery increasing with further hyperpolarization and higher extracellular K+. Inactivation was also reversed when the intracellular Ca2+ concentration was lowered to 100 nM and was permanently removed by application of trypsin to the inner patch surface. In addition, inactivation was perturbed by application of either tetraethylammonium ions or the Shaker (Sh)B peptide to the inner membrane face. 4. During inactivation, channel Po was greater at hyperpolarized rather than depolarized potentials, which was partly the result of a greater number of longer duration openings. Depolarizing voltage steps (-40 to +40 mV) applied during longer duration openings produced only short duration events at the depolarized potential, yielding a transient ensemble average current with a rapid decay (tau, approximately 3.8 ms). 5. These data suggest that hippocampal BK channels exhibit a Ca2+-dependent inactivation that is proposed to result from block of the channel by an associated particle. The findings that inactivation was removed by trypsin and prolonged by decreasing extracellular potassium suggest that the blocking particle may act at the intracellular side of the channel.

Activation and two modes of blockade by strontium of Ca2+-activated K+ channels in goldfish saccular hair cells

Effects of internal Sr2+ on the activity of large-conductance Ca2+-activated K+ channels were studied in inside-out membrane patches from goldfish saccular hair cells. Sr2+ was approximately one-fourth as potent as Ca2+ in activating these channels. Although the Hill coefficient for Sr2+ was smaller than that for Ca2+, maximum open-state probability, voltage dependence, steady state gating kinetics, and time courses of activation and deactivation of the channel were very similar under the presence of equipotent concentrations of Ca2+ and Sr2+. This suggests that voltage-dependent activation is partially independent of the ligand. Internal Sr2+ at higher concentrations (>100 microM) produced fast and slow blockade both concentration and voltage dependently. The reduction in single-channel amplitude (fast blockade) could be fitted with a modified Woodhull equation that incorporated the Hill coefficient. The dissociation constant at 0 mV, the Hill coefficient, and zd (a product of the charge of the blocking ion and the fraction of the voltage difference at the binding site from the inside) in this equation were 58-209 mM, 0.69-0.75, 0.45-0.51, respectively (n = 4). Long shut events (slow blockade) produced by Sr2+ lasted approximately 10-200 ms and could be fitted with single-exponential curves (time constant, taul-s) in shut-time histograms. Durations of burst events, periods intercalated by long shut events, could also be fitted with single exponentials (time constant, taub). A significant decrease in taub and no large changes in taul-s were observed with increased Sr2+ concentration and voltage. These findings on slow blockade could be approximated by a model in which single Sr2+ ions bind to a blocking site within the channel pore beyond the energy barrier from the inside, as proposed for Ba2+ blockade. The dissociation constant at 0 mV and zd in the Woodhull equation for this model were 36-150 mM and 1-1.8, respectively (n = 3).

Time-irreversible subconductance gating associated with Ba2+ block of large conductance Ca2+-activated K+ channels

Ba2+ block of large conductance Ca2+-activated K+ channels was studied in patches of membrane excised from cultures of rat skeletal muscle using the patch clamp technique. Under conditions in which a blocking Ba2+ ion would dissociate to the external solution (150 mM N-methyl-D-glucamine+o, 500 mM K+i, 10 microM Ba2+i, +30 mV, and 100 microM Ca2+i to fully activate the channel), Ba2+ blocks with a mean duration of approximately 2 s occurred, on average, once every approximately 100 ms of channel open time. Of these Ba2+ blocks, 78% terminated with a single step in the current to the fully open level and 22% terminated with a transition to a subconductance level at approximately 0.26 of the fully open level (preopening) before stepping to the fully open level. Only one apparent preclosing was observed in approximately 10,000 Ba2+ blocks. Thus, the preopenings represent Ba2+-induced time-irreversible subconductance gating. The fraction of Ba2+ blocks terminating with a preopening and the duration of preopenings (exponentially distributed, mean = 0.75 ms) appeared independent of changes in [Ba2+]i or membrane potential. The fractional conductance of the preopenings increased from 0.24 at +10 mV to 0.39 at +90 mV. In contrast, the average subconductance level during normal gating in the absence of Ba2+ was independent of membrane potential, suggesting different mechanisms for preopenings and normal subconductance levels. Preopenings were also observed with 10 mM Ba2+o and no added Ba2+i. Adding K+, Rb+, or Na+ to the external solution decreased the fraction of Ba2+ blocks with preopenings, with K+ and Rb+ being more effective than Na+. These results are consistent with models in which the blocking Ba2+ ion either induces a preopening gate, and then dissociates to the external solution, or moves to a site located on the external side of the Ba2+ blocking site and acts directly as the preopening gate.

Potassium channels in the vasculature

Many important cellular functions are regulated by vascular potassium channels, including the resting membrane potential. Recent evidence suggests that the function of these channels is altered in pathophysiological disorders of the cardiovascular system. Using molecular cloning techniques, considerable effort has been made over the past 5 years to elucidate the structure of various types of potassium channels. Several different potassium channel clones have been identified from neuronal and cardiac tissues, although only a few have so far been identified in smooth muscle.

A novel type of internal barium block of a maxi-K+ channel from human vas deferens epithelial cells

We have recently shown that a maxi-K+ channel from vas deferens epithelial cells contains two Ba2+-binding sites accessible from the external side: a "flickering" site located deep in the channel pore and a "slow" site located close to the extracellular mouth of the channel. Using the patch-clamp technique, we have now studied the effect of internal Ba2+ on this channel. Cytoplasmic Ba2+ produced a voltage- and concentration-dependent "slow" type of block with a dissociation constant of approximately 100 microM. However, based on its voltage dependence and sensitivity to K+ concentration, this block was clearly different from the external "slow" Ba2+ block previously described. Kinetic analysis also revealed a novel "fast flickering" block restricted to channel bursts, with an unblocking rate of approximately 310 s(-1), some 10-fold faster than the external "flickering" block. Taken together, these results show that this channel contains multiple Ba2+-binding sites within the conduction pore. We have incorporated this information into a new model of Ba2+ block, a novel feature of which is that internal "slow" block results from the binding of at least two Ba2+ ions. Our results suggest that current models for Ba2+ block of maxi-K+ channels need to be revised.

Redox modulation of hslo Ca2+-activated K+ channels

The modulation of ion channel proteins by cellular redox potential has emerged recently as a significant determinant of channel function. We have investigated the influence of sulfhydryl redox reagents on human brain Ca2+-activated K+ channels (hslo) expressed in both human embryonic kidney 293 cells and Xenopus oocytes using macropatch and single-channel analysis. Intracellular application of the reducing agent dithiothreitol (DTT): (1) shifts the voltage of half-maximal channel activation (V0.5) approximately 18 mV to more negative potentials without affecting the maximal conductance or the slope of the voltage dependence; (2) slows by approximately 10-fold a time-dependent right-shift in V0.5 values ("run-down"); (3) speeds macroscopic current activation kinetics by approximately 33%; and (4) increases the single-channel open probability without affecting the unitary conductance. In contrast to DTT treatment, oxidation with hydrogen peroxide shifts macropatch V0.5 values to more positive potentials, increases the rate of channel run-down, and decreases the single-channel open probability. KCa channels cloned from Drosophila differ from hslo channels in that they show very little run-down and are not modulated by the addition of DTT. These data indicate that hslo Ca2+-activated K+ channels may be modulated by changes in the cellular redox potential as well as by the transmembrane voltage and the cytoplasmic Ca2+ concentration.

Redox modulation of hslo Ca2+-activated K+ channels

The modulation of ion channel proteins by cellular redox potential has emerged recently as a significant determinant of channel function. We have investigated the influence of sulfhydryl redox reagents on human brain Ca2+-activated K+ channels (hslo) expressed in both human embryonic kidney 293 cells and Xenopus oocytes using macropatch and single-channel analysis. Intracellular application of the reducing agent dithiothreitol (DTT): (1) shifts the voltage of half-maximal channel activation (V0.5) approximately 18 mV to more negative potentials without affecting the maximal conductance or the slope of the voltage dependence; (2) slows by approximately 10-fold a time-dependent right-shift in V0.5 values ("run-down"); (3) speeds macroscopic current activation kinetics by approximately 33%; and (4) increases the single-channel open probability without affecting the unitary conductance. In contrast to DTT treatment, oxidation with hydrogen peroxide shifts macropatch V0.5 values to more positive potentials, increases the rate of channel run-down, and decreases the single-channel open probability. KCa channels cloned from Drosophila differ from hslo channels in that they show very little run-down and are not modulated by the addition of DTT. These data indicate that hslo Ca2+-activated K+ channels may be modulated by changes in the cellular redox potential as well as by the transmembrane voltage and the cytoplasmic Ca2+ concentration.

Intrinsic voltage dependence and Ca2+ regulation of mslo large conductance Ca-activated K+ channels

The kinetic and steady-state properties of macroscopic mslo Ca-activated K+ currents were studied in excised patches from Xenopus oocytes. In response to voltage steps, the timecourse of both activation and deactivation, but for a brief delay in activation, could be approximated by a single exponential function over a wide range of voltages and internal Ca2+ concentrations ([Ca]i). Activation rates increased with voltage and with [Ca]i, and approached saturation at high [Ca]i. Deactivation rates generally decreased with [Ca]i and voltage, and approached saturation at high [Ca]i. Plots of the macroscopic conductance as a function of voltage (G-V) and the time constant of activation and deactivation shifted leftward along the voltage axis with increasing [Ca]i. G-V relations could be approximated by a Boltzmann function with an equivalent gating charge which ranged between 1.1 and 1.8 e as [Ca]i varied between 0.84 and 1,000 microM. Hill analysis indicates that at least three Ca2+ binding sites can contribute to channel activation. Three lines of evidence indicate that there is at least one voltage-dependent unimolecular conformational change associated with mslo gating that is separate from Ca2+ binding. (a) The position of the mslo G-V relation does not vary logarithmically with [Ca]i. (b) The macroscopic rate constant of activation approaches saturation at high [Ca]i but remains voltage dependent. (c) With strong depolarizations mslo currents can be nearly maximally activated without binding Ca2+. These results can be understood in terms of a channel which must undergo a central voltage-dependent rate limiting conformational change in order to move from closed to open, with rapid Ca2+ binding to both open and closed states modulating this central step.

Separation of gating properties from permeation and block in mslo large conductance Ca-activated K+ channels

In this and the following paper we have examined the kinetic and steady-state properties of macroscopic mslo Ca-activated K+ currents in order to interpret these currents in terms of the gating behavior of the mslo channel. To do so, however, it was necessary to first find conditions by which we could separate the effects that changes in Ca2+ concentration or membrane voltage have on channel permeation from the effects these stimuli have on channel gating. In this study we investigate three phenomena which are unrelated to gating but are manifest in macroscopic current records: a saturation of single channel current at high voltage, a rapid voltage-dependent Ca2+ block, and a slow voltage-dependent Ba2+ block. Where possible methods are described by which these phenomena can be separated from the effects that changes in Ca2+ concentration and membrane voltage have on channel gating. Where this is not possible, some assessment of the impact these effects have on gating parameters determined from macroscopic current measurements is provided. We have also found that without considering the effects of Ca2+ and voltage on channel permeation and block, macroscopic current measurements suggest that mslo channels do not reach the same maximum open probability at all Ca2+ concentrations. Taking into account permeation and blocking effects, however, we find that this is not the case. The maximum open probability of the mslo channel is the same or very similar over a Ca2+ concentration range spanning three orders of magnitude indicating that over this range the internal Ca2+ concentration does not limit the ability of the channel to be activated by voltage.

A Ba2+ chelator suppresses long shut events in fully activated high-conductance Ca(2+)-dependent K+ channels

High-conductance Ca(2+)-activated K+ channels from rat skeletal muscle were incorporated into planar lipid bilayers, and the channel kinetics were studied with a high internal Ca2+ concentration (Cai). Raising the Cai is known to increase the channel open probability. This effect is due to an increases in openings frequency and duration, and saturates at a Cai around 100 microM. Raising the Cai also increases the occurrence of less frequent but very long (> 5 s) shut events. The mechanism underlying this slow kinetic process was studied. Raising Cai above 100 microM does not further increase the frequency of the long shut events. This was not consistent with the hypothesis that the long closures result from a classical channel-block mechanism induced by internal Ca2+. The transmembrane voltage and the presence of K+ ions in the external compartment both affect the slow kinetic process. A comparison of these effects with the properties of the channel block induced by Ba2+ ions added to the internal compartment strongly suggested that the long shut events are due to a contamination of the internal solutions by Ba2+. This was confirmed by showing that a crown-ether compound that strongly chelates Ba2+ completely suppresses the long shut events when added to the inner compartment.

Kinetic variability and modulation of dSlo, a cloned calcium-dependent potassium channel

We have examined, using patch recording, the modulation by ATP gamma S of the cloned Drosophila slopoke calcium-dependent potassium channel (dSlo) expressed in Xenopus oocytes. There is a large variation in the gating kinetics, open probability, and conductance level of the channel in this expression system, which complicates the analysis of modulatory events. Addition of ATP gamma S to the intracellular face of the patch does not consistently alter the overall open probability of dSlo, but it does increase the frequency of appearance of an exceptionally long-lived closed state of the channel. This modulation is not blocked by an inhibitor of several serine/threonine protein kinases, nor by mutation of a serine residue that is a target for phosphorylation by protein kinase A. Thus, ATP gamma S may alter dSlo kinetic properties by some mechanism other than serine/threonine phosphorylation.