Large conductance, Ca(2+)- and voltage-activated K(+) channels (BK) respond to two distinct physiological signals -- membrane voltage and cytosolic Ca(2+) (refs 1, 2). Channel opening is regulated by changes in Ca(2+) concentration spanning 0.5 micro M to 50 mM (refs 2-5), a range of Ca(2+) sensitivity unusual among Ca(2+)-regulated proteins. Although voltage regulation arises from mechanisms shared with other voltage-gated channels, the mechanisms of Ca(2+) regulation remain largely unknown. One potential Ca(2+)-regulatory site, termed the 'Ca(2+) bowl', has been located to the large cytosolic carboxy terminus. Here we show that a second region of the C terminus, the RCK domain (regulator of conductance for K(+) (ref. 12)), contains residues that define two additional regulatory effects of divalent cations. One site, together with the Ca(2+) bowl, accounts for all physiological regulation of BK channels by Ca(2+); the other site contributes to effects of millimolar divalent cations that may mediate physiological regulation by cytosolic Mg(2+) (refs 5, 13). Independent regulation by multiple sites explains the large concentration range over which BK channels are regulated by Ca(2+). This allows BK channels to serve a variety of physiological roles contingent on the Ca(2+) concentration to which the channels are exposed.

Mouse spermatozoa express a pH-dependent K + current (KSper) thought to be composed of subunits encoded by the Slo3 gene. However, the equivalence of KSper and Slo3-dependent current remains uncertain, because heterologous expression of Slo3 results in currents that are less effectively activated by alkalization than are native KSper currents. Here, we show that genetic deletion of Slo3 abolishes all pH-dependent K + current at physiological membrane potentials in corpus epididymal sperm. A residual pH-dependent outward current (I Kres ) is observed in Slo3 −/− sperm at potentials of >0 mV. Differential inhibition of KSper/Slo3 and I Kres by clofilium reveals that the amplitude of I Kres is similar in both wild-type (wt) and Slo3 −/− sperm. The properties of I Kres suggest that it likely represents outward monovalent cation flux through CatSper channels. Thus, KSper/Slo3 may account for essentially all mouse sperm K + current and is the sole pH-dependent K + conductance in these sperm. With physiological ionic gradients, alkalization depolarizes Slo3 −/− spermatozoa, presumably from CatSper activation, in contrast to Slo3/KSper-mediated hyperpolarization in wt sperm. Slo3 −/− male mice are infertile, but Slo3 −/− sperm exhibit some fertility within in vitro fertilization assays. Slo3 −/− sperm exhibit a higher incidence of morphological abnormalities accentuated by hypotonic challenge and also exhibit deficits in motility in the absence of bicarbonate, revealing a role of KSper under unstimulated conditions. Together, these results show that KSper/Slo3 is the primary spermatozoan K + current, that KSper may play a critical role in acquisition of normal morphology and sperm motility when faced with hyperosmotic challenges, and that Slo3 is critical for fertility.

A family of accessory beta subunits significantly contributes to the functional diversity of large-conductance, Ca(2+)- and voltage-dependent potassium (BK) channels in native cells. Here we describe the functional properties of one variant of the beta subunit family, which confers properties on BK channels totally unlike any that have as yet been observed. Coexpression of this subunit (termed beta3) with Slo alpha subunits results in rectifying outward currents and, at more positive potentials, rapidly inactivating ( approximately 1 msec) currents. The underlying rapid inactivation process results in an increase in the apparent activation rate of macroscopic currents, which is coupled with a shift in the activation range of the currents at low Ca(2+). As a consequence, the currents exhibit more rapid activation at low Ca(2+) relative to any other BK channel subunit combinations that have been examined. In part because of the rapid inactivation process, single channel openings are exceedingly brief. Although variance analysis suggests a conductance in excess of 160 pS, fully resolved single channel openings are not observed. The inactivation process results from a cytosolic N-terminal domain of the beta3 subunit, whereas an extended C-terminal domain does not participate in the inactivation process. Thus, the beta3 subunit appears to use a rapid inactivation mechanism to produce a current with a relatively rapid apparent activation time course at low Ca(2+). The beta3 subunit is a compelling example of how the beta subunit family can finely tune the gating properties of Ca(2+)- and voltage-dependent BK channels.

Mutational analyses have suggested that BK channels are regulated by three distinct divalent cation-dependent regulatory mechanisms arising from the cytosolic COOH terminus of the pore-forming α subunit. Two mechanisms account for physiological regulation of BK channels by μM Ca2+. The third may mediate physiological regulation by mM Mg2+. Mutation of five aspartate residues (5D5N) within the so-called Ca2+ bowl removes a portion of a higher affinity Ca2+ dependence, while mutation of D362A/D367A in the first RCK domain also removes some higher affinity Ca2+ dependence. Together, 5D5N and D362A/D367A remove all effects of Ca2+ up through 1 mM while E399A removes a portion of low affinity regulation by Ca2+/Mg2+. If each proposed regulatory effect involves a distinct divalent cation binding site, the divalent cation selectivity of the actual site that defines each mechanism might differ. By examination of the ability of various divalent cations to activate currents in constructs with mutationally altered regulatory mechanisms, here we show that each putative regulatory mechanism exhibits a unique sensitivity to divalent cations. Regulation mediated by the Ca2+ bowl can be activated by Ca2+ and Sr2+, while regulation defined by D362/D367 can be activated by Ca2+, Sr2+, and Cd2+. Mn2+, Co2+, and Ni2+ produce little observable effect through the high affinity regulatory mechanisms, while all six divalent cations enhance activation through the low affinity mechanism defined by residue E399. Furthermore, each type of mutation affects kinetic properties of BK channels in distinct ways. The Ca2+ bowl mainly accelerates activation of BK channels at low [Ca2+], while the D362/D367-related high affinity site influences both activation and deactivation over the range of 10–300 μM Ca2+. The major kinetic effect of the E399-related low affinity mechanism is to slow deactivation at mM Mg2+ or Ca2+. The results support the view that three distinct divalent-cation binding sites mediate regulation of BK channels.

KSper, a pH-dependent K + current in mouse spermatozoa that is critical for fertility, is activated by alkalization in the range of pH 6.4-7.2 at membrane potentials between −50 and 0 mV. Although the KSper pore-forming subunit is encoded by the Slo3 gene, heterologously expressed Slo3 channels are largely closed at potentials negative to 0 mV at physiological pH. Here we identify a Slo3-associating protein, LRRC52 (leucine-rich repeat-containing 52), that shifts Slo3 gating into a range of voltages and pH values similar to that producing KSper current activation. Message for LRRC52, a homolog of the Slo1-modifying LRRC26 protein, is enriched in testis relative to other homologous LRRC subunits and is developmentally regulated in concert with that for Slo3. LRRC52 protein is detected only in testis. It is markedly diminished from Slo3 −/− testis and completely absent from Slo3 −/− sperm, indicating that LRRC52 expression is critically dependent on the presence of Slo3. We also examined the ability of other LRRC subunits homologous to LRRC26 and LRRC52 to modify Slo3 currents. Although both LRRC26 and LRRC52 are able to modify Slo3 function, LRRC52 is the stronger modifier of Slo3 function. Effects of other related subunits were weaker or absent. We propose that LRRC52 is a testis-enriched Slo3 auxiliary subunit that helps define the specific alkalization dependence of KSper activation. Together, LRRC52 and LRRC26 define a new family of auxiliary subunits capable of critically modifying the gating behavior of Slo family channels.

The mouse Slo3 gene (KCNMA3) encodes a K+ channel that is regulated by changes in cytosolic pH. Like Slo1 subunits responsible for the Ca2+ and voltage-activated BK-type channel, the Slo3 α subunit contains a pore module with homology to voltage-gated K+ channels and also an extensive cytosolic C terminus thought to be responsible for ligand dependence. For the Slo3 K+ channel, increases in cytosolic pH promote channel activation, but very little is known about many fundamental properties of Slo3 currents. Here we define the dependence of macroscopic conductance on voltage and pH and, in particular, examine Slo3 conductance activated at negative potentials. Using this information, the ability of a Horrigan-Aldrich–type of general allosteric model to account for Slo3 gating is examined. Finally, the pH and voltage dependence of Slo3 activation and deactivation kinetics is reported. The results indicate that Slo3 differs from Slo1 in several important ways. The limiting conductance activated at the most positive potentials exhibits a pH-dependent maximum, suggesting differences in the limiting open probability at different pH. Furthermore, over a 600 mV range of voltages (−300 to +300 mV), Slo3 conductance shifts only about two to three orders of magnitude, and the limiting conductance at negative potentials is relatively voltage independent compared to Slo1. Within the context of the Horrigan-Aldrich model, these results indicate that the intrinsic voltage dependence (zL) of the Slo3 closed–open equilibrium and the coupling (D) between voltage sensor movement are less than in Slo1. The kinetic behavior of Slo3 currents also differs markedly from Slo1. Both activation and deactivation are best described by two exponential components, both of which are only weakly voltage dependent. Qualitatively, the properties of the two kinetic components in the activation time course suggest that increases in pH increase the fraction of more rapidly opening channels.

A family of auxiliary β subunits coassemble with Slo α subunit to form Ca2+-regulated, voltage-activated BK-type K+ channels. The β subunits play an important role in regulating the functional properties of the resulting channel protein, including apparent Ca2+ dependence and inactivation. The β3b auxiliary subunit, when coexpressed with the Slo α subunit, results in a particularly rapid (∼1 ms), but incomplete inactivation, mediated by the cytosolic NH2 terminus of the β3b subunit (Xia et al. 2000). Here, we evaluate whether a simple block of the open channel by the NH2-terminal domain accounts for the inactivation mechanism. Analysis of the onset of block, recovery from block, time-dependent changes in the shape of instantaneous current-voltage curves, and properties of deactivation tails suggest that a simple, one step blocking reaction is insufficient to explain the observed currents. Rather, blockade can be largely accounted for by a two-step blocking mechanism () in which preblocked open states (O*n) precede blocked states (In). The transitions between O* and I are exceedingly rapid accounting for an almost instantaneous block or unblock of open channels observed with changes in potential. However, the macroscopic current relaxations are determined primarily by slower transitions between O and O*. We propose that the O to O* transition corresponds to binding of the NH2-terminal inactivation domain to a receptor site. Blockade of current subsequently reflects either additional movement of the NH2-terminal domain into a position that hinders ion permeation or a gating transition to a closed state induced by binding of the NH2 terminus.

Large-conductance Ca(2+)-activated K(+) (BK) channels can regulate cellular excitability in complex ways because they are able to respond independently to two distinct cellular signals, cytosolic Ca(2+) and membrane potential. In rat chromaffin cells (RCC), inactivating BK(i) and noninactivating (BK(s)) channels differentially contribute to RCC action potential (AP) firing behavior. However, the basis for these differential effects has not been fully established. Here, we have simulated RCC action potential behavior, using Markovian models of BK(i) and BK(s) current and other RCC currents. The analysis shows that BK current influences both fast hyperpolarization and afterhyperpolarization of single APs and that, consistent with experimental observations, BK(i) current facilitates repetitive firing of APs, whereas BK(s) current does not. However, the key functional difference between BK(i) and BK(s) current that accounts for the differential firing is not inactivation but the more negatively shifted activation range for BK(i) current at a given [Ca(2+)].