Negatively charged residues adjacent to IFM motif in the DIII-DIV linker of hNa(V)1.4 differentially affect slow inactivation

The effects on slow inactivation (SI) of charge substitutions, neutralizations, and reversals were studied for the negatively charged residues D1309 and EE1314,15 surrounding the IFM motif in the DIII-DIV cytoplasmic linker - the putative fast inactivation particle - of human skeletal muscle voltage-gated sodium channel (hNa(V)1.4). Changing aspartate (D) at position 1309 to glutamate (E) (substitution) did not strongly affect SI, whereas charge neutralization to glutamine (Q) and charge reversal to arginine (R) right-shifted the midpoint of the steady-state SI curve. Charge neutralization (D-->Q) at position 1309 also reduced the apparent valence associated with SI. Glutamates (E) at positions 1314 and 1315 were similarly mutated. Charge reversal (EE-->RR) right-shifted the steady-state SI curve and both reversal and substitution (EE-->DD) reduced its apparent valence. Charge neutralization (EE-->QQ) and reversal decreased the maximum probability of SI. These mutations also had differential effects on the rate of SI onset and recovery. These results suggest that charged residues in the DIII-DIV linker may interact with structures that control SI.     

Modulation of voltage sensitivity by N-terminal cytoplasmic residues in human Kv1.2 channels

Potassium channels are now among the best understood membrane proteins and most salient functions have been mapped onto distinct portions of the protein. The detailed mechanism by which movement of the voltage sensor is transduced into channel opening is yet to be understood. We have constructed chimaeras from our collection of human voltage-gated potassium channels and expressed them in Xenopus oocytes. Here we report on a chimaeric construct, 1N/2, generated by swapping the N-terminal cytoplasmic residues of hKv1.1 onto the transmembrane body of hKv1.2. This chimaera functions as a classic outward rectifier but with a 25 mV hyperpolarizing shift in the mid-point of channel activation. The conductance of oocytes expressing this construct decreases significantly on depolarizing beyond +5 mV, unlike full-length hKv1.2. Other parameters such as ionic selectivity and charybdotoxin blockage are unaffected in making the chimaera. These observations suggest that the introduction of the "foreign" chain from hKv1.1 does not cause a large-scale perturbation of channel structure. Loss of the N-terminus from hKv1.2 is not responsible for the shift in voltage dependence, as a truncation construct, delta75N2, starting at the splice junction, has the same voltage-dependence as full-length hKv1.2. Both constructs show a maximum in their conductance-voltage curves. This decline in conductance on extensive depolarization may arise due to perturbations to the machinery that locks channels into their open state on depolarization. Taken together with our observations on other N-terminal swapped chimaeras, our data imply that N-terminal residues can interact with transmembrane regions and perturb the machinery mediating voltage-dependent channel gating.     

Sequence differences in the IQ motifs of CaV1.1 and CaV1.2 strongly impact calmodulin binding and calcium-dependent inactivation

The proximal C terminus of the cardiac L-type calcium channel (Ca(V)1.2) contains structural elements important for the binding of calmodulin (CaM) and calcium-dependent inactivation, and exhibits extensive sequence conservation with the corresponding region of the skeletal L-type channel (Ca(V)1.1). However, there are several Ca(V)1.1 residues that are both identical in six species and are non-conservatively changed from the corresponding Ca(V)1.2 residues, including three of the "IQ motif." To investigate the functional significance of these residue differences, we used native gel electrophoresis and expression in intact myotubes to compare the binding of CaM to extended regions (up to 300 residues) of the C termini of Ca(V)1.1 and Ca(V)1.2. We found that in the presence of Ca(2+) (either millimolar or that in resting myotubes), CaM bound strongly to C termini of Ca(V)1.2 but not of Ca(V)1.1. Furthermore, replacement of two residues (Tyr(1657) and Lys(1662)) within the IQ motif of a C-terminal Ca(V)1.2 construct with the divergent residues of Ca(V)1.1 (His(1532) and Met(1537)) led to a weakening of CaM binding (native gels), whereas the reciprocal substitution in Ca(V)1.1 caused a gain of CaM binding. In full-length Ca(V)1.2, substitution of these same two divergent residues with those of Ca(V)1.1 (Y1657H, K1662M) eliminated calcium-dependent inactivation of the heterologously expressed channel. Thus, our results reveal that a conserved difference between the IQ motifs of Ca(V)1.2 and Ca(V)1.1 has a profound effect on both CaM binding and calcium-dependent inactivation.     

Role of putative voltage-sensor countercharge D4 in regulating gating properties of CaV1.2 and CaV1.3 calcium channels

Voltage-dependent calcium channels (Ca_V) activate over a wide range of membrane potentials, and the voltage-dependence of activation of specific channel isoforms is exquisitely tuned to their diverse functions in excitable cells. Alternative splicing further adds to the stunning diversity of gating properties. For example, developmentally regulated insertion of an alternatively spliced exon 29 in the fourth voltage-sensing domain (VSD IV) of Ca_V1.1 right-shifts voltage-dependence of activation by 30 mV and decreases the current amplitude several-fold. Previously we demonstrated that this regulation of gating properties depends on interactions between positive gating charges (R1, R2) and a negative countercharge (D4) in VSD IV of Ca_V1.1. Here we investigated whether this molecular mechanism plays a similar role in the VSD IV of Ca_V1.3 and in VSDs II and IV of Ca_V1.2 by introducing charge-neutralizing mutations (D4N or E4Q) in the corresponding positions of Ca_V1.3 and in two splice variants of Ca_V1.2. In both channels the D4N (VSD IV) mutation resulted in a ?5 mV right-shift of the voltage-dependence of activation and in a reduction of current density to about half of that in controls. However in Ca_V1.2 the effects were independent of alternative splicing, indicating that the two modulatory processes operate by distinct mechanisms. Together with our previous findings these results suggest that molecular interactions engaging D4 in VSD IV contribute to voltage-sensing in all examined Ca_V1 channels, however its striking role in regulating the gating properties by alternative splicing appears to be a unique property of the skeletal muscle Ca_V1.1 channel.     

Sodium channel gating in clonal pituitary cells. The inactivation step is not voltage dependent

We have determined the time course of Na channel inactivation in clonal pituitary (GH3) cells by comparing records before and after the enzymatic removal of inactivation. The cells were subjected to whole-cell patch clamp, with papain included in the internal medium. Inactivation was slowly removed over the course of 10 min, making it possible to obtain control records before the enzyme acted. Papain caused a large (4-100x) increase in current magnitude for small depolarizations (near -40 mV), and a much smaller increase for large ones (approximately 1.5x at +40 mV). For technical reasons it was sometimes convenient to study outward INa recorded with no Na+ outside. The instantaneous I-V (IIV) curve in this condition was nonlinear before papain, and more nearly linear afterwards. The gNa-V curve after papain, obtained by dividing the INa-V curve by the IIV curve, was left-shifted by at least 20 mV and steepened. A spontaneous 5-10 mV left shift occurred in the absence of papain. The rate of the inactivation step was found to vary only slightly from -100 mV to +60 mV, based on the following evidence. (a) Before papain, inactivation rate saturated with voltage and was constant from +20 to +60 mV. (b) We activated the channels with a brief pulse, and studied the time course of the current on changing the voltage to a second, usually more negative level (Na+ present internally and externally). The time course of inactivation at each voltage was obtained by comparing control traces with those after inactivation was removed. When the 5-10-mV spontaneous shift was taken into account, inactivation rate changed by less than 10% from -100 to +60 mV. The data are considered in terms of existing models of the Na channel.     

Roles of molecular regions in determining differences between voltage dependence of activation of CaV3.1 and CaV1.2 calcium channels

Voltage-dependent calcium channels are classified into low voltage-activated and high voltage-activated channels. We have investigated the molecular basis for this difference in voltage dependence of activation by constructing chimeras between a low voltage-activated channel (Ca(V)3.1) and a high voltage-activated channel (Ca(V)1.2), focusing on steady-state activation properties. Wild type and chimeras were expressed in oocytes, and two-electrode voltage clamp recordings were made of calcium channel currents. Replacement of domains I, III, or IV of the Ca 3.1 channel with the corresponding domain of Ca(V)1.2 led (V)to high voltage-activated channels; for these constructs the current/voltage (I/V) curves were similar to those for Ca(V)1.2 wild type. However, replacement of domain II gave only a small shift to the right of the I/V curve and modulation of the activation kinetics but did not lead to a high voltage-activating channel with an I/V curve like Ca 1.2. We also investigated the role of the voltage sensor (V)S4 by replacing the S4 segment of Ca(V)3.1 with that of Ca 1.2. For domain I, there was no shift in the I/V curve (V)as compared with Ca(V)3.1, and there were relatively small shifts to the right for domains III and IV. Taken together, these results suggest that domains I, III, and IV (rather than domain II) are apparently critical for channel opening and, therefore, contribute strongly to the difference in voltage dependence of activation between Ca 3.1 and Ca(V)1.2. However, the S4 segments in domains I, (V)III, and IV did not account for this difference in voltage dependence.     

Contributions of charged residues in a cytoplasmic linking region to Na channel gating

Na channels inactivate quickly after opening, and the very highly positively charged cytoplasmic linking region between homologous domains III and IV of the channel molecule acts as the inactivation gate. To test the hypothesis that the charged residues in the domain III to domain IV linker have a role in channel function, we measured currents through wild-type and two mutant skeletal muscle Na channels expressed in Xenopus oocytes, each lacking two or three charged residues in the inactivation gate. Microscopic current measures showed that removing charges hastened activation and inactivation. Macroscopic current measures showed that removing charges altered the voltage dependence of inactivation, suggesting less coupling of the inactivation and activation processes. Reduced intracellular ionic strength shifted the midpoint of equilibrium activation gating to a greater extent, and shifted the midpoint of equilibrium inactivation gating to a lesser extent in the mutant channels. The results allow the possibility that an electrostatic mechanism contributes to the role of charged residues in Na channel inactivation gating.     

Resistance of presynaptic CaV2.2 channels to voltage-dependent inactivation: dynamic palmitoylation and voltage sensitivity

Presynaptic CaV2.2 (N type) calcium channels gate the influx of calcium ions to trigger transmitter release. We have previously demonstrated at the chick ciliary ganglion presynaptic calyx terminal that the bulk of these channels are highly resistant to voltage dependent inactivation [E.F. Stanley, G. Goping, Characterization of a calcium current in a vertebrate cholinergic presynaptic nerve terminal, J. Neurosci. 11 (1991) 985-993; E.F. Stanley, Syntaxin I modulation of presynaptic calcium channel inactivation revealed by botulinum toxin C1, Eur. J. Neurosci. 17 (2003) 1303-1305; E.F. Stanley, R.R. Mirotznik, Cleavage of syntaxin prevents G-protein regulation of presynaptic calcium channels, Nature (Lond.) 385 (1997) 340-343]. Recent studies have suggested that CaV2.2 can be rendered inactivation resistant when expressed with the palmitoylated beta2A subunit and that this effect can be eliminated by tunicamycin, a general inhibitor of dynamic palmitoylation [J.H. Hurley, A.L. Cahill, K.P. Currie, A.P. Fox, The role of dynamic palmitoylation in Ca(2+) channel inactivation, Proc. Natl. Acad. Sci. U.S.A. 97 (2000) 9293-9298]. We find that while tunicamycin treatment had no effect on CaV2.2 current in the inactivation-sensitive isolated chick dorsal root ganglion (DRG) neuron, it caused a 10mV hyperpolarized shift in the profile of the inactivation-resistant presynaptic CaV2.2 population. This shift occurred without any effect on the voltage sensitivity of the inactivation process, as measured by a Boltzmann slope factor. Our findings suggest that dynamic palmitoylation contributes to the hyperpolarized steady inactivation profile of presynaptic CaV2.2. However, some other factor must also contribute since its inhibition does is not restore the inactivation profile to that of channels in the cell soma.     

The role of distal S6 hydrophobic residues in the voltage-dependent gating of CaV2.3 channels

The hydrophobic locus VAVIM is conserved in the S6 transmembrane segment of domain IV (IVS6) in Ca(V)1 and Ca(V)2 families. Herein we show that glycine substitution of the VAVIM motif in Ca(V)2.3 produced whole cell currents with inactivation kinetics that were either slower (A1719G approximately V1720G), similar (V1718G), or faster (I1721G approximately M1722G) than the wild-type channel. The fast kinetics of I1721G were observed with a approximately +10 mV shift in its voltage dependence of activation (E(0.5,act)). In contrast, the slow kinetics of A1719G and V1720G were accompanied by a significant shift of approximately -20 mV in their E(0.5,act) indicating that the relative stability of the channel closed state was decreased in these mutants. Glycine scan performed with Val (349) in IS6, Ile(701) in IIS6, and Leu(1420) in IIIS6 at positions predicted to face Val(1720) in IVS6 also produced slow inactivating currents with hyperpolarizing shifts in the activation and inactivation potentials, again pointing out a decrease in the stability of the channel closed state. Mutations to other hydrophobic residues at these positions nearly restored the channel gating. Altogether these data indicate that residues at positions equivalent to 1720 exert a critical control upon the relative stability of the channel closed and open states and more specifically, that hydrophobic residues at these positions promote the channel closed state. We discuss a three-dimensional homology model of Ca(V)2.3 based upon Kv1.2 where hydrophobic residues at positions facing Val(1720) in IS6, IIS6, and IIIS6 play a critical role in stabilizing the closed state in Ca(V)2.3.     

Negatively charged residues in the IgM stop-transfer effector sequence regulate transmembrane polypeptide integration

A non-hydrophobic sequence that contributes to the biogenesis of a transmembrane protein is termed a stop-transfer effector (STE). To examine the mechanism of STE-mediated stop-transfer, a series of fusion proteins were constructed containing variants of a putative STE from murine IgM fused to an otherwise translocated hydrophobic sequence. Unexpectedly, the fraction of molecules adopting transmembrane topology was insensitive to many amino acid substitutions within the STE sequence but varied directly with the number of negative charges. Furthermore, when present at the amino terminus of a reporter, mutants were observed that adopted type I (amino terminus lumenal) and type II (amino terminus cytoplasmic) transmembrane topologies, demonstrating that the STE sequence can be located at either side of the endoplasmic reticulum membrane. Our results suggest that recognition of a broad structural feature formed primarily by negatively charged residues within the STE halts translocation and triggers membrane integration, even when the negative charges end up on the cytoplasmic side of the membrane. Since functional STE sequences photocross-link to two membrane proteins not previously identified at the translocon, these unique proteins are presumably involved in recognizing STE sequences and/or facilitating STE function.     

The Na channel voltage sensor associated with inactivation is localized to the external charged residues of domain IV, S4.

Site-3 toxins have been shown to inhibit a component of gating charge (33% of maximum gating charge, Q(max)) in native cardiac Na channels that has been identified with the open-to-inactivated state kinetic transition. To investigate the role of the three outermost arginine amino acid residues in segment 4 domain IV (R1, R2, R3) in gating charge inhibited by site-3 toxins, we recorded ionic and gating currents from human heart Na channels with mutations of the outermost arginines (R1C, R1Q, R2C, and R3C) expressed in fused, mammalian tsA201 cells. All four mutations had ionic currents that activated over the same voltage range with slope factors of their peak conductance-voltage (G-V) relationships similar to those of wild-type channels, although decay of I(Na) was slowest for R1C and R1Q mutant channels and fastest for R3C mutant channels. After Na channel modification by Ap-A toxin, decays of I(Na) were slowed to similar values for all four channel mutants. Toxin modification produced a graded effect on gating charge (Q) of mutant channels, reducing Q(max) by 12% for the R1C and R1Q mutants, by 22% for the R2C mutant, and by 27% for the R3C mutant, only slightly less than the 31% reduction seen for wild-type currents. Consistent with these findings, the relationship of Q(max) to G(max) was significantly shallower for R1 mutants than for R2C and R3C mutant Na channels. These data suggest that site-3 toxins primarily inhibit gating charge associated with movement of the S4 in domain IV, and that the outermost arginine contributes the largest amount to channel gating, with other arginines contributing less.     

Negatively charged residues in the membrane ordering activity of SARS-CoV-1 and -2 fusion peptides

Entry of coronaviruses into host cells is mediated by the viral spike protein. Previously, we identified the bona fide fusion peptides (FPs) for severe acute respiratory syndrome coronavirus (“SARS-1”) and severe acute respiratory syndrome coronavirus-2 (“SARS-2”) using electron spin resonance spectroscopy. We also found that their FPs induce membrane ordering in a Ca²⁺-dependent fashion. Here we study which negatively charged residues in SARS-1 FP are involved in this binding, to build a topological model and clarify the role of Ca²⁺. Our systematic mutation study on the SARS-1 FP shows that all six negatively charged residues contribute to the FP’s membrane ordering activity, with D812 the dominant residue. The corresponding SARS-2 residue D830 plays an equivalent role. We provide a topological model of how the FP binds Ca²⁺ ions: its two segments FP1 and FP2 each bind one Ca²⁺. The binding of Ca²⁺, the folding of FP (both studied by isothermal titration calorimetry experiments), and the ordering activity correlate very well across the mutants, suggesting that the Ca²⁺ helps the folding of FP in membranes to enhance the ordering activity. Using a novel pseudotyped viral particle-liposome methodology, we monitored the membrane ordering induced by the FPs in the whole spike protein in its trimer form in real time. We found that the SARS-1 and SARS-2 pseudotyped viral particles also induce membrane ordering to the extent that separate FPs do, and mutations of the negatively charged residues also significantly suppress the membrane ordering activity. However, the slower kinetics of the FP ordering activity versus that of the pseudotyped viral particle suggest the need for initial trimerization of the FPs.     

A single charged voltage sensor is capable of gating the Shaker K+ channel

We sought to determine the contribution of an individual voltage sensor to Shaker''s function. Concatenated heterotetramers of Shaker zH4 Δ(6–46) wild type (wt) in combination with a neutral S4 segment Shaker mutant (mut) with stoichiometries 2wt/2mut and 1wt/3mut were studied and compared with the 4wt concatenated homotetramer. A single charged voltage sensor is sufficient to open Shaker conductance with reduced delay (<1 ms) and at more hyperpolarized voltages compared with 4wt. In addition, the wt-like slow inactivation of 1wt/3mut was almost completely eliminated by mutations T449V-I470C in its single wt subunit, indicating that the subunits bearing a neutral S4 were unable to trigger slow inactivation. Our results strongly suggest that a neutral S4 segment of Shaker''s subunit is voltage insensitive and its voltage sensor is in the activated position (i.e., ready for pore opening), and provide experimental support to the proposed model of independent voltage sensors with a final, almost voltage-independent concerted step.     

Negatively charged residues and hydrogen bonds tune the ligand histidine pKa values of Rieske iron-sulfur proteins

Rieske proteins carry a redox-active iron-sulfur cluster, which is bound by two histidine and two cysteine side chains. The reduction potential of Rieske proteins depends on pH. This pH dependence can be described by two pK(a) values, which have been assigned to the two iron-coordinating histidines. Rieske proteins are commonly grouped into two major classes: Rieske proteins from quinol-oxidizing cytochrome bc complexes, in which the ligand histidines titrate in the physiological pH range, and bacterial ferredoxin Rieske proteins, in which the ligand histidines are protonated at physiological pH. In the study presented here, we have calculated pK(a) values of the cluster ligand histidines using a combined density functional theory/continuum electrostatics approach. Experimental pK(a) values for a bc-type and a ferredoxin Rieske protein could be reproduced. We could identify functionally important differences between the two proteins: hydrogen bonds toward the cluster, which are present in bc-type Rieske proteins, and negatively charged residues, which are present in ferredoxin Rieske proteins. We removed these differences by mutating the proteins in our calculations. The Rieske centers in the mutated proteins have very similar pK(a) values. We thus conclude that the studied structural differences are the main reason for the different pH-titration behavior of the proteins. Interestingly, the shift caused by neutralizing the negative charges in ferredoxin Rieske proteins is larger than the shift caused by removing the hydrogen bonds toward the cluster in bc-type Rieske proteins.     

A gating charge interaction required for late slow inactivation of the bacterial sodium channel NavAb

Voltage-gated sodium channels undergo slow inactivation during repetitive depolarizations, which controls the frequency and duration of bursts of action potentials and prevents excitotoxic cell death. Although homotetrameric bacterial sodium channels lack the intracellular linker-connecting homologous domains III and IV that causes fast inactivation of eukaryotic sodium channels, they retain the molecular mechanism for slow inactivation. Here, we examine the functional properties and slow inactivation of the bacterial sodium channel NavAb expressed in insect cells under conditions used for structural studies. NavAb activates at very negative membrane potentials (V_1/2 of approximately −98 mV), and it has both an early phase of slow inactivation that arises during single depolarizations and reverses rapidly, and a late use-dependent phase of slow inactivation that reverses very slowly. Mutation of Asn49 to Lys in the S2 segment in the extracellular negative cluster of the voltage sensor shifts the activation curve ∼75 mV to more positive potentials and abolishes the late phase of slow inactivation. The gating charge R3 interacts with Asn49 in the crystal structure of NavAb, and mutation of this residue to Cys causes a similar positive shift in the voltage dependence of activation and block of the late phase of slow inactivation as mutation N49K. Prolonged depolarizations that induce slow inactivation also cause hysteresis of gating charge movement, which results in a requirement for very negative membrane potentials to return gating charges to their resting state. Unexpectedly, the mutation N49K does not alter hysteresis of gating charge movement, even though it prevents the late phase of slow inactivation. Our results reveal an important molecular interaction between R3 in S4 and Asn49 in S2 that is crucial for voltage-dependent activation and for late slow inactivation of NavAb, and they introduce a NavAb mutant that enables detailed functional studies in parallel with structural analysis.     

A slow component of gating current in crayfish giant axons resembles inactivation charge movement.

Recent experimental evidence from a number of preparations indicates that sodium channel inactivation may be intrinsically voltage sensitive. Intrinsically voltage sensitive inactivation should produce a charge movement. Crayfish giant axons provide a unique opportunity to reexamine the slower components of gating currents (Ig) for a contribution from inactivation (Igh). In reference to other axon preparations, this preparation has relatively rapid inactivation, and steady-state inactivation has a comparatively steep voltage dependence. As predicted by a two-state scheme for voltage-sensitive sodium channel inactivation, Ig in crayfish axons includes a slow component with time constant comparable to the time constant of decay of the sodium current. Allowing for some delay in its onset (60 microseconds), inactivation as described by this slow component of Ig carries roughly the amount of charge predicted by the voltage dependence of inactivation.     

Two components of voltage-dependent inactivation in Ca(v)1.2 channels revealed by its gating currents

Voltage-dependent inactivation (VDI) was studied through its effects on the voltage sensor in Ca(v)1.2 channels expressed in tsA 201 cells. Two kinetically distinct phases of VDI in onset and recovery suggest the presence of dual VDI processes. Upon increasing duration of conditioning depolarizations, the half-distribution potential (V(1/2)) of intramembranous mobile charge was negatively shifted as a sum of two exponential terms, with time constants 0.5 s and 4 s, and relative amplitudes near 50% each. This kinetics behavior was consistent with that of increment of maximal charge related to inactivation (Qn). Recovery from inactivation was also accompanied by a reduction of Qn that varied with recovery time as a sum of two exponentials. The amplitudes of corresponding exponential terms were strongly correlated in onset and recovery, indicating that channels recover rapidly from fast VDI and slowly from slow VDI. Similar to charge "immobilization," the charge moved in the repolarization (OFF) transient became slower during onset of fast VDI. Slow VDI had, instead, hallmarks of interconversion of charge. Confirming the mechanistic duality, fast VDI virtually disappeared when Li(+) carried the current. A nine-state model with parallel fast and slow inactivation pathways from the open state reproduces most of the observations.     

From the gating charge response to pore domain movement: Initial motions of Kv1.2 dynamics under physiological voltage changes

Abstract

Recent structures of the potassium channel provide an essential beginning point for explaining how the pore is gated between open and closed conformations by changes in membrane voltage. Yet, the molecular details of this process and the connections to transmembrane gradients are not understood. To begin addressing how changes within a membrane environment lead to the channel’s ability to sense shifts in membrane voltage and to gate, we performed double-bilayer simulations of the Kv1.2 channel. These double-bilayer simulations enable us to simulate realistic voltage drops from resting potential conditions to depolarized conditions by changes in the bath conditions on each side of the bilayer. Our results show how the voltage sensor domain movement responds to differences in transmembrane potential. The initial voltage sensor domain movement, S4 in particular, is modulated by the gating charge response to changes in voltage and is initially stabilized by the lipid headgroups. We show this response is directly coupled to the initial stages of pore domain motion. Results presented here provide a molecular model for how the pre-gating process occurs in sequential steps: Gating charge response, movement and stabilization of the S4 voltage sensor domain, and movement near the base of the S5 region to close the pore domain.     

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.