Heme regulates allosteric activation of the Slo1 BK channel

Large conductance calcium-dependent (Slo1 BK) channels are allosterically activated by membrane depolarization and divalent cations, and possess a rich modulatory repertoire. Recently, intracellular heme has been identified as a potent regulator of Slo1 BK channels (Tang, X.D., R. Xu, M.F. Reynolds, M.L. Garcia, S.H. Heinemann, and T. Hoshi. 2003. Nature. 425:531-535). Here we investigated the mechanism of the regulatory action of heme on heterologously expressed Slo1 BK channels by separating the influences of voltage and divalent cations. In the absence of divalent cations, heme generally decreased ionic currents by shifting the channel's G-V curve toward more depolarized voltages and by rendering the curve less steep. In contrast, gating currents remained largely unaffected by heme. Simulations suggest that a decrease in the strength of allosteric coupling between the voltage sensor and the activation gate and a concomitant stabilization of the open state account for the essential features of the heme action in the absence of divalent ions. At saturating levels of divalent cations, heme remained similarly effective with its influence on the G-V simulated by weakening the coupling of both Ca(2+) binding and voltage sensor activation to channel opening. The results thus show that heme dampens the influence of allosteric activators on the activation gate of the Slo1 BK channel. To account for these effects, we consider the possibility that heme binding alters the structure of the RCK gating ring and thereby disrupts both Ca(2+)- and voltage-dependent gating as well as intrinsic stability of the open state.     

An S6 mutation in BK channels reveals beta1 subunit effects on intrinsic and voltage-dependent gating

Large conductance, Ca(2+)- and voltage-activated K(+) (BK) channels are exquisitely regulated to suit their diverse roles in a large variety of physiological processes. BK channels are composed of pore-forming alpha subunits and a family of tissue-specific accessory beta subunits. The smooth muscle-specific beta1 subunit has an essential role in regulating smooth muscle contraction and modulates BK channel steady-state open probability and gating kinetics. Effects of beta1 on channel's gating energetics are not completely understood. One of the difficulties is that it has not yet been possible to measure the effects of beta1 on channel's intrinsic closed-to-open transition (in the absence of voltage sensor activation and Ca(2+) binding) due to the very low open probability in the presence of beta1. In this study, we used a mutation of the alpha subunit (F315Y) that increases channel openings by greater than four orders of magnitude to directly compare channels' intrinsic open probabilities in the presence and absence of the beta1 subunit. Effects of beta1 on steady-state open probabilities of both wild-type alpha and the F315Y mutation were analyzed using the dual allosteric HA model. We found that mouse beta1 has two major effects on channel's gating energetics. beta1 reduces the intrinsic closed-to-open equilibrium that underlies the inhibition of BK channel opening seen in submicromolar Ca(2+). Further, P(O) measurements at limiting slope allow us to infer that beta1 shifts open channel voltage sensor activation to negative membrane potentials, which contributes to enhanced channel opening seen at micromolar Ca(2+) concentrations. Using the F315Y alpha subunit with deletion mutants of beta1, we also demonstrate that the small N- and C-terminal intracellular domains of beta1 play important roles in altering channel's intrinsic opening and voltage sensor activation. In summary, these results demonstrate that beta1 has distinct effects on BK channel intrinsic gating and voltage sensor activation that can be functionally uncoupled by mutations in the intracellular domains.     

Gating and ionic currents reveal how the BKCa channel's Ca2+ sensitivity is enhanced by its beta1 subunit

Large-conductance Ca(2+)-activated K(+) channels (BK(Ca) channels) are regulated by the tissue-specific expression of auxiliary beta subunits. Beta1 is predominantly expressed in smooth muscle, where it greatly enhances the BK(Ca) channel's Ca(2+) sensitivity, an effect that is required for proper regulation of smooth muscle tone. Here, using gating current recordings, macroscopic ionic current recordings, and unitary ionic current recordings at very low open probabilities, we have investigated the mechanism that underlies this effect. Our results may be summarized as follows. The beta1 subunit has little or no effect on the equilibrium constant of the conformational change by which the BK(Ca) channel opens, and it does not affect the gating charge on the channel's voltage sensors, but it does stabilize voltage sensor activation, both when the channel is open and when it is closed, such that voltage sensor activation occurs at more negative voltages with beta1 present. Furthermore, beta1 stabilizes the active voltage sensor more when the channel is closed than when it is open, and this reduces the factor D by which voltage sensor activation promotes opening by approximately 24% (16.8-->12.8). The effects of beta1 on voltage sensing enhance the BK(Ca) channel's Ca(2+) sensitivity by decreasing at most voltages the work that Ca(2+) binding must do to open the channel. In addition, however, in order to fully account for the increase in efficacy and apparent Ca(2+) affinity brought about by beta1 at negative voltages, our studies suggest that beta1 also decreases the true Ca(2+) affinity of the closed channel, increasing its Ca(2+) dissociation constant from approximately 3.7 microM to between 4.7 and 7.1 microM, depending on how many binding sites are affected.     

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.     

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.     

A role for the S0 transmembrane segment in voltage-dependent gating of BK channels

BK (Maxi-K) channel activity is allosterically regulated by a Ca2+ sensor, formed primarily by the channel's large cytoplasmic carboxyl tail segment, and a voltage sensor, formed by its transmembrane helices. As with other voltage-gated K channels, voltage sensing in the BK channel is accomplished through interactions of the S1-S4 transmembrane segments with the electric field. However, the BK channel is unique in that it contains an additional amino-terminal transmembrane segment, S0, which is important in the functional interaction between BK channel alpha and beta subunits. In this study, we used perturbation mutagenesis to analyze the role of S0 in channel gating. Single residues in the S0 region of the BK channel were substituted with tryptophan to give a large change in side chain volume; native tryptophans in S0 were substituted with alanine. The effects of the mutations on voltage- and Ca2+-dependent gating were quantified using patch-clamp electrophysiology. Three of the S0 mutants (F25W, L26W, and S29W) showed especially large shifts in their conductance-voltage (G-V) relations along the voltage axis compared to wild type. The G-V shifts for these mutants persisted at nominally 0 Ca2+, suggesting that these effects cannot arise simply from altered Ca2+ sensitivity. The basal open probabilities for these mutants at hyperpolarized voltages (where voltage sensor activation is minimal) were similar to wild type, suggesting that these mutations may primarily perturb voltage sensor function. Further analysis using the dual allosteric model for BK channel gating showed that the major effects of the F25W, L26W, and S29W mutations could be accounted for primarily by decreasing the equilibrium constant for voltage sensor movement. We conclude that S0 may make functional contact with other transmembrane regions of the BK channel to modulate the equilibrium between resting and active states of the channel's voltage sensor.     

Differential effects of beta 1 and beta 2 subunits on BK channel activity

High conductance, calcium- and voltage-activated potassium (BK) channels are widely expressed in mammals. In some tissues, the biophysical properties of BK channels are highly affected by coexpression of regulatory (beta) subunits. beta1 and beta2 subunits increase apparent channel calcium sensitivity. The beta1 subunit also decreases the voltage sensitivity of the channel and the beta2 subunit produces an N-type inactivation of BK currents. We further characterized the effects of the beta1 and beta2 subunits on the calcium and voltage sensitivity of the channel, analyzing the data in the context of an allosteric model for BK channel activation by calcium and voltage (Horrigan and Aldrich, 2002). In this study, we used a beta2 subunit without its N-type inactivation domain (beta2IR). The results indicate that the beta2IR subunit, like the beta1 subunit, has a small effect on the calcium binding affinity of the channel. Unlike the beta1 subunit, the beta2IR subunit also has no effect on the voltage sensitivity of the channel. The limiting voltage dependence for steady-state channel activation, unrelated to voltage sensor movements, is unaffected by any of the studied beta subunits. The same is observed for the limiting voltage dependence of the deactivation time constant. Thus, the beta1 subunit must affect the voltage sensitivity by altering the function of the voltage sensors of the channel. Both beta subunits reduce the intrinsic equilibrium constant for channel opening (L0). In the allosteric activation model, the reduction of the voltage dependence for the activation of the voltage sensors accounts for most of the macroscopic steady-state effects of the beta1 subunit, including the increase of the apparent calcium sensitivity of the BK channel. All allosteric coupling factors need to be increased in order to explain the observed effects when the alpha subunit is coexpressed with the beta2IR subunit.     

The contribution of RCK domains to human BK channel allosteric activation

Large conductance voltage- and Ca(2+)-activated K(+) (BK) channels are potent regulators of cellular processes including neuronal firing, synaptic transmission, cochlear hair cell tuning, insulin release, and smooth muscle tone. Their unique activation pathway relies on structurally distinct regulatory domains including one transmembrane voltage-sensing domain (VSD) and two intracellular high affinity Ca(2+)-sensing sites per subunit (located in the RCK1 and RCK2 domains). Four pairs of RCK1 and RCK2 domains form a Ca(2+)-sensing apparatus known as the "gating ring." The allosteric interplay between voltage- and Ca(2+)-sensing apparati is a fundamental mechanism of BK channel function. Using voltage-clamp fluorometry and UV photolysis of intracellular caged Ca(2+), we optically resolved VSD activation prompted by Ca(2+) binding to the gating ring. The sudden increase of intracellular Ca(2+) concentration ([Ca(2+)](i)) induced a hyperpolarizing shift in the voltage dependence of both channel opening and VSD activation, reported by a fluorophore labeling position 202, located in the upper side of the S4 transmembrane segment. The neutralization of the Ca(2+) sensor located in the RCK2 domain abolished the effect of [Ca(2+)](i) increase on the VSD rearrangements. On the other hand, the mutation of RCK1 residues involved in Ca(2+) sensing did not prevent the effect of Ca(2+) release on the VSD, revealing a functionally distinct interaction between RCK1 and RCK2 and the VSD. A statistical-mechanical model quantifies the complex thermodynamics interplay between Ca(2+) association in two distinct sites, voltage sensor activation, and BK channel opening.     

Mg2+ enhances voltage sensor/gate coupling in BK channels

BK (Slo1) potassium channels are activated by millimolar intracellular Mg(2+) as well as micromolar Ca(2+) and membrane depolarization. Mg(2+) and Ca(2+) 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 Mg(2+) action is highly dependent on voltage sensor activation and therefore differs fundamentally from that of Ca(2+). Evidence that Ca(2+) 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 microM Ca(2+) increases P(O) more than 15-fold at -120 mV. However 10 mM Mg(2+), which has an effect on the G(K)-V relation similar to 2 microM Ca(2+), has no detectable effect on P(O) when voltage sensors are in the resting state. Gating currents are only slightly altered by Mg(2+) when channels are closed, indicating that Mg(2+) does not act merely to promote voltage sensor activation. Indeed, channel opening is facilitated in a voltage-independent manner by Mg(2+) in a mutant (R210C) whose voltage sensors are constitutively activated. Thus, 10 mM Mg(2+) increases P(O) only when voltage sensors are activated, effectively strengthening the allosteric coupling of voltage sensor activation to channel opening. Increasing Mg(2+) from 10 to 100 mM, to occupy very low affinity binding sites, has additional effects on gating that more closely resemble those of Ca(2+). The effects of Mg(2+) on steady-state activation and I(K) kinetics are discussed in terms of an allosteric gating scheme and the state-dependent interactions between Mg(2+) and voltage sensor that may underlie this mechanism.     

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

The activation of large conductance Ca(2+)-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 (tau(I(K))) over an extended voltage range in 0-50 microM [Ca(2+)](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 tau(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.     

Functional coupling of the beta(1) subunit to the large conductance Ca(2+)-activated K(+) channel in the absence of Ca(2+). Increased Ca(2+) sensitivity from a Ca(2+)-independent mechanism

Coexpression of the beta(1) subunit with the alpha subunit (mSlo) of BK channels increases the apparent Ca(2+) sensitivity of the channel. This study investigates whether the mechanism underlying the increased Ca(2+) sensitivity requires Ca(2+), by comparing the gating in 0 Ca(2+)(i) of BK channels composed of alpha subunits to those composed of alpha+beta(1) subunits. The beta(1) subunit increased burst duration approximately 20-fold and the duration of gaps between bursts approximately 3-fold, giving an approximately 10-fold increase in open probability (P(o)) in 0 Ca(2+)(i). The effect of the beta(1) subunit on increasing burst duration was little changed over a wide range of P(o) achieved by varying either Ca(2+)(i) or depolarization. The effect of the beta(1) subunit on increasing the durations of the gaps between bursts in 0 Ca(2+)(i) was preserved over a range of voltage, but was switched off as Ca(2+)(i) was increased into the activation range. The Ca(2+)-independent, beta(1) subunit-induced increase in burst duration accounted for 80% of the leftward shift in the P(o) vs. Ca(2+)(i) curve that reflects the increased Ca(2+) sensitivity induced by the beta(1) subunit. The Ca(2+)-dependent effect of the beta(1) subunit on the gaps between bursts accounted for the remaining 20% of the leftward shift. Our observation that the major effects of the beta(1) subunit are independent of Ca(2+)(i) suggests that the beta(1) subunit mainly alters the energy barriers of Ca(2+)-independent transitions. The changes in gating induced by the beta(1) subunit differ from those induced by depolarization, as increasing P(o) by depolarization or by the beta(1) subunit gave different gating kinetics. The complex gating kinetics for both alpha and alpha+beta(1) channels in 0 Ca(2+)(i) arise from transitions among two to three open and three to five closed states and are inconsistent with Monod-Wyman-Changeux type models, which predict gating among only one open and one closed state in 0 Ca(2+)(i).     

Mg(2+) binding to open and closed states can activate BK channels provided that the voltage sensors are elevated

BK channels are activated by intracellular Ca(2+) and Mg(2+) as well as by depolarization. Such activation is possible because each of the four subunits has two high-affinity Ca(2+) sites, one low-affinity Mg(2+) site, and a voltage sensor. This study further investigates the mechanism of Mg(2+) activation by using single-channel recording to determine separately the action of Mg(2+) on the open and closed states of the channel. To limit Mg(2+) action to the Mg(2+) sites, the two high-affinity Ca(2+) sites are disabled by mutation. When the voltage is stepped from negative holding potentials to +100 mV, we find that 10 mM Mg(2+) decreases the mean closed latency to the first channel opening 2.1-fold, decreases the mean closed interval duration 8.7-fold, increases mean burst duration 10.1-fold, increases the number of openings per burst 4.4-fold, and increases mean open interval duration 2.3-fold. Hence, Mg(2+) can bind to closed BK channels, increasing their opening rates, and to open BK channels, decreasing their closing rates. To explore the relationship between Mg(2+) action and voltage sensor activation, we record single-channel activity in macropatches containing hundreds of channels. Open probability (P(o)) is dramatically increased by 10 mM Mg(2+) when voltage sensors are activated with either depolarization or the mutation R210C. The increased P(o) arises from large decreases in mean closed interval durations and moderate increases in mean open interval durations. In contrast, 10 mM Mg(2+) has no detectable effects on P(o) or interval durations when voltage sensors are deactivated with very negative potentials or the mutation R167E. These observations are consistent with a model in which Mg(2+) can bind to and alter the gating of both closed and open states to increase P(o), provided that one or more voltage sensors are activated.     

Intra- and intersubunit cooperativity in activation of BK channels by Ca2+

The activation of BK channels by Ca(2+) is highly cooperative, with small changes in intracellular Ca(2+) concentration having large effects on open probability (Po). Here we examine the mechanism of cooperative activation of BK channels by Ca(2+). Each of the four subunits of BK channels has a large intracellular COOH terminus with two different high-affinity Ca(2+) sensors: an RCK1 sensor (D362/D367) located on the RCK1 (regulator of conductance of K(+)) domain and a Ca-bowl sensor located on or after the RCK2 domain. To determine interactions among these Ca(2+) sensors, we examine channels with eight different configurations of functional high-affinity Ca(2+) sensors on the four subunits. We find that the RCK1 sensor and Ca bowl contribute about equally to Ca(2+) activation of the channel when there is only one high-affinity Ca(2+) sensor per subunit. We also find that an RCK1 sensor and a Ca bowl on the same subunit are much more effective in increasing Po than when they are on different subunits, indicating positive intrasubunit cooperativity. If it is assumed that BK channels have a gating ring similar to MthK channels with alternating RCK1 and RCK2 domains and that the Ca(2+) sensors act at the flexible (rather than fixed) interfaces between RCK domains, then a comparison of the distribution of Ca(2+) sensors with the observed responses suggest that the interface between RCK1 and RCK2 domains on the same subunit is flexible. On this basis, intrasubunit cooperativity arises because two high-affinity Ca(2+) sensors acting across a flexible interface are more effective in opening the channel than when acting at separate interfaces. An allosteric model incorporating intrasubunit cooperativity nested within intersubunit cooperativity could approximate the Po vs. Ca(2+) response for eight possible subunit configurations of the high-affinity Ca(2+) sensors as well as for three additional configurations from a previous study.     

The NH2 terminus of RCK1 domain regulates Ca2+-dependent BK(Ca) channel gating

Large conductance, voltage- and Ca2+-activated K+ (BK(Ca)) channels regulate blood vessel tone, synaptic transmission, and hearing owing to dual activation by membrane depolarization and intracellular Ca2+. Similar to an archeon Ca2+-activated K+ channel, MthK, each of four alpha subunits of BK(Ca) may contain two cytosolic RCK domains and eight of which may form a gating ring. The structure of the MthK channel suggests that the RCK domains reorient with one another upon Ca2+ binding to change the gating ring conformation and open the activation gate. Here we report that the conformational changes of the NH2 terminus of RCK1 (AC region) modulate BK(Ca) gating. Such modulation depends on Ca2+ occupancy and activation states, but is not directly related to the Ca2+ binding sites. These results demonstrate that AC region is important in the allosteric coupling between Ca2+ binding and channel opening. Thus, the conformational changes of the AC region within each RCK domain is likely to be an important step in addition to the reorientation of RCK domains leading to the opening of the BK(Ca) activation gate. Our observations are consistent with a mechanism for Ca2+-dependent activation of BK(Ca) channels such that the AC region inhibits channel activation when the channel is at the closed state in the absence of Ca2+; Ca2+ binding and depolarization relieve this inhibition.     

Modes of operation of the BKCa channel beta2 subunit

The beta(2) subunit of the large conductance Ca(2+)- and voltage-activated K(+) channel (BK(Ca)) modulates a number of channel functions, such as the apparent Ca(2+)/voltage sensitivity, pharmacological and kinetic properties of the channel. In addition, the N terminus of the beta(2) subunit acts as an inactivating particle that produces a relatively fast inactivation of the ionic conductance. Applying voltage clamp fluorometry to fluorescently labeled human BK(Ca) channels (hSlo), we have investigated the mechanisms of operation of the beta(2) subunit. We found that the leftward shift on the voltage axis of channel activation curves (G(V)) produced by coexpression with beta(2) subunits is associated with a shift in the same direction of the fluorescence vs. voltage curves (F(V)), which are reporting the voltage dependence of the main voltage-sensing region of hSlo (S4-transmembrane domain). In addition, we investigated the inactivating mechanism of the beta(2) subunits by comparing its properties with the ones of the typical N-type inactivation process of Shaker channel. While fluorescence recordings from the inactivated Shaker channels revealed the immobilization of the S4 segments in the active conformation, we did not observe a similar feature in BK(Ca) channels coexpressed with the beta(2) subunit. The experimental observations are consistent with the view that the beta(2) subunit of BK(Ca) channels facilitates channel activation by changing the voltage sensor equilibrium and that the beta(2)-induced inactivation process does not follow a typical N-type mechanism.     

Functional effects of auxiliary beta4-subunit on rat large-conductance Ca(2+)-activated K(+) channel

Large-conductance calcium-activated potassium (BK(Ca)) channels are composed of the pore-forming alpha-subunit and the auxiliary beta-subunits. The beta4-subunit is dominantly expressed in the mammalian central nervous system. To understand the physiological roles of the beta4-subunit on the BK(Ca) channel alpha-subunit (Slo), we isolated a full-length complementary DNA of rat beta4-subunit (rbeta4), expressed heterolgously in Xenopus oocytes, and investigated the detailed functional effects using electrophysiological means. When expressed together with rat Slo (rSlo), rbeta4 profoundly altered the gating characteristics of the Slo channel. At a given concentration of intracellular Ca(2+), rSlo/rbeta4 channels were more sensitive to transmembrane voltage changes. The activation and deactivation rates of macroscopic currents were decreased in a Ca(2+)-dependent manner. The channel activation by Ca(2+) became more cooperative by the coexpression of rbeta4. Single-channel recordings showed that the increased Hill coefficient for Ca(2+) was due to the changes in the open probability of the rSlo/rbeta4 channel. Single BK(Ca) channels composed of rSlo and rbeta4 also exhibited slower kinetics for steady-state gating compared with rSlo channels. Dwell times of both open and closed events were significantly increased. Because BK(Ca) channels are known to modulate neuroexcitability and the expression of the beta4-subunit is highly concentrated in certain subregions of brain, the electrophysiological properties of individual neurons should be affected profoundly by the expression of this second subunit.     

(Xeno)estrogen sensitivity of smooth muscle BK channels conferred by the regulatory beta1 subunit: a study of beta1 knockout mice

Estrogen and xenoestrogens (i.e. agents that are not steroids but possess estrogenic activity) increase the open probability (P(o)) of large conductance Ca(2+)-activated K(+) (BK) channels in smooth muscle. The mechanism of action may involve the regulatory beta1 subunit. We used beta1 subunit knockout (beta1-/-) mice to test the hypothesis that the regulatory beta1 subunit is essential for the activation of BK channels by tamoxifen, 4-OH tamoxifen (a major biologically active metabolite), and 17beta-estradiol in native myocytes. Patch clamp recordings demonstrate BK channels from beta1-/- mice were similar to wild type with the exception of markedly reduced Ca(2+)/voltage sensitivity and faster activation kinetics. In wild type myocytes, (xeno)estrogens increased NP(o) (P(o) x the number of channels, N), shifted the voltage of half-activation (V(12)) to more negative potentials, and decreased unitary conductance. These effects were non-genomic and direct, because they were rapid, reversible, and observed in cell-free patches. None of the (xeno)estrogens increased the NP(o) of BK channels from beta1-/- mice, but all three agents decreased single channel conductance. Thus, (xeno)estrogens increase BK NP(o) through a mechanism involving the beta1 subunit. The decrease in conductance did not require the beta1 subunit and probably reflects an interaction with the pore-forming alpha subunit. We demonstrate regulation of smooth muscle BK channels by physiological (steroid hormones) and pharmacological (chemotherapeutic) agents and reveal the critical role of the beta1 subunit in these responses in native myocytes.     

Homology modeling identifies C-terminal residues that contribute to the Ca2+ sensitivity of a BKCa channel

Activation of BK(Ca) channels by direct Ca(2+) binding and membrane depolarization occur via independent and additive molecular processes. The "calcium bowl" domain is critically involved in Ca(2+)-dependent gating, and we have hypothesized that a sequence within this domain may resemble an EF hand motif. Using a homology modeling strategy, it was observed that a single Ca(2+) ion may be coordinated by the oxygen-containing side chains of residues within the calcium bowl (i.e., (912)ELVNDTNVQFLD(923)). To examine these predictions directly, alanine-substituted BK(Ca) channel mutants were expressed in HEK 293 cells and the voltage and Ca(2+) dependence of macroscopic currents were examined in inside-out membrane patches. Over the range of 1-10 microM free Ca(2+), single point mutations (i.e., E912A and D923A) produced rightward shifts in the steady-state conductance-voltage relations, whereas the mutants N918A or Q920A had no effect on Ca(2+)-dependent gating. The double mutant E912A/D923A displayed a synergistic shift in Ca(2+)-sensitive gating, as well as altered kinetics of current activation/deactivation. In the presence of 1, 10, and 80 mM cytosolic Mg(2+), this double mutation significantly reduced the Ca(2+)-induced free energy change associated with channel activation. Finally, mutations that altered sensitivity of the holo-channel to Ca(2+) also reduced direct (45)Ca binding to the calcium bowl domain expressed as a bacterial fusion protein. These findings, along with other recent data, are considered in the context of the calcium bowl's high affinity Ca(2+) sensor and the known properties of EF hands.     

The influence exerted by the beta(3) subunit on MVIIA omega-conotoxin binding to neuronal N-type calcium channels

In the present study, two-electrode voltage-clamp techniques have been used to assess the interaction between the MVIIA omega-conotoxin and an isoform of the N-type Ca(2+) channel alpha subunit (alpha(1B-d)). Cloned alpha(1B-d) Ca(2+) channels were expressed in Xenopus laevis oocytes in the presence and absence of the beta(3) subunit. Coexpression of the beta(3) subunit significantly shifted the IC(50) value for MVIIA inhibition of central N-type Ca(2+) channel current. Analysis of the peak conductance vs. depolarising voltage dependence suggested that the beta(3) subunit has no apparent effect on the gating charge which accompanies the closed-open transition of the channels. Instead, coexpression of the beta(3) subunit led to an approx. 10 mV shift to more hyperpolarised potentials in the voltage-dependent activation of N-type Ca(2+) channels. We conclude that MVIIA alters the surface charge on the N-type Ca(2+) channels and might induce allosteric changes on the structure of the channel, leading to an increase in the dissociation constant of MVIIA binding.     

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.