S4 charges move close to residues in the pore domain during activation in a K channel.

Voltage-gated ion channels respond to changes in the transmembrane voltage by opening or closing their ion conducting pore. The positively charged fourth transmembrane segment (S4) has been identified as the main voltage sensor, but the mechanisms of coupling between the voltage sensor and the gates are still unknown. Obtaining information about the location and the exact motion of S4 is an important step toward an understanding of these coupling mechanisms. In previous studies we have shown that the extracellular end of S4 is located close to segment 5 (S5). The purpose of the present study is to estimate the location of S4 charges in both resting and activated states. We measured the modification rates by differently charged methanethiosulfonate regents of two residues in the extracellular end of S5 in the Shaker K channel (418C and 419C). When S4 moves to its activated state, the modification rate by the negatively charged sodium (2-sulfonatoethyl) methanethiosulfonate (MTSES(-)) increases significantly more than the modification rate by the positively charged [2-(trimethylammonium)ethyl] methanethiosulfonate, bromide (MTSET(+)). This indicates that the positive S4 charges are moving close to 418C and 419C in S5 during activation. Neutralization of the most external charge of S4 (R362), shows that R362 in its activated state electrostatically affects the environment at 418C by 19 mV. In contrast, R362 in its resting state has no effect on 418C. This suggests that, during activation of the channel, R362 moves from a position far away (>20 A) to a position close (8 A) to 418C. Despite its close approach to E418, a residue shown to be important in slow inactivation, R362 has no effect on slow inactivation or the recovery from slow inactivation. This refutes previous models for slow inactivation with an electrostatic S4-to-gate coupling. Instead, we propose a model with an allosteric mechanism for the S4-to-gate coupling.     

Probing the outer vestibule of a sodium channel voltage sensor.

The second and third basic residues of the S4 segment of domain 4 (D4:R2 and D4:R3) of the human skeletal muscle Na+ channel are known to be translocated from a cytoplasmic to an extracellular position during depolarization. Accessibilities of individual S4 residues were assayed by alteration of inactivation kinetics during modification of cysteine mutants by hydrophilic methanethiosulfonate reagents. The voltage dependences of the reaction rates are identical for extracellular application of cationic methanethiosulfonate-ethyltrimethylammonium (MTSET) and anionic methanethiosulfonate-ethylsulfonate (MTSES), suggesting that D4:R3C is situated outside the membrane electric field at depolarized voltages. The absolute rate of R3C modification is 281-fold greater for MTSET than for MTSES, however, suggesting that at depolarized voltages this S4 thiol resides in a negatively charged hydrophilic crevice. The two hydrophobic residues between D4:R2C and D4:R3C in the primary sequence (L1452 and A1453) are not externally exposed at any voltage. An alpha-helical representation of D4/S4 shows that the basic residues D4:R2 and D4:R3 are on the face opposite that of L1452 and A1453. We propose that in the depolarized conformation, the hydrophobic face of this portion of D4/S4 remains in contact with a hydrophobic region of the extracellular vestibule of the S4 channel.     

Outer pore topology of the ECaC-TRPV5 channel by cysteine scan mutagenesis

The substituted cysteine accessibility method (SCAM) was used to map the external vestibule and the pore region of the ECaC-TRPV5 calcium-selective channel. Cysteine residues were introduced at 44 positions from the end of S5 (Glu515) to the beginning of S6 (Ala560). Covalent modification by positively charged MTSET applied from the external medium significantly inhibited whole cell currents at 15/44 positions. Strongest inhibition was observed in the S5-linker to pore region (L520C, G521C, and E522C) with either MTSET or MTSES suggesting that these residues were accessible from the external medium. In contrast, the pattern of covalent modification by MTSET for residues between Pro527 and Ile541 was compatible with the presence of a alpha-helix. The absence of modification by the negatively charged MTSES in that region suggests that the pore region has been optimized to favor the entrance of positively charged ions. Cysteine mutants at positions -1, 0, +1, +2 around Asp542 (high Ca2+ affinity site) were non-functional. Whole cell currents of cysteine mutants at +4 and +5 positions were however covalently inhibited by external MTSET and MTSES. Altogether, the pattern of covalent modification by MTS reagents globally supports a KcsA homology-based three-dimensional model whereby the external vestibule in ECaC-TRPV5 encompasses three structural domains consisting of a coiled structure (Glu515 to Tyr526) connected to a small helical segment of 15 amino acids (527PTALFSTFELFLT539) followed by two distinct coiled structures Ile540-Pro544 (selectivity filter) and Ala545-Ile557 before the beginning of S6.     

The drug-binding pocket of the human multidrug resistance P-glycoprotein is accessible to the aqueous medium

P-Glycoprotein (P-gp) is an ATP-dependent drug pump that transports a broad range of compounds out of the cell. Cross-linking studies have shown that the drug-binding pocket is at the interface between the transmembrane (TM) domains and can simultaneously bind two different drug substrates. Here, we determined whether cysteine residues within the drug-binding pocket were accessible to the aqueous medium. Cysteine mutants were tested for their reactivity with the charged thiol-reactive compounds sodium (2-sulfonatoethyl)methanethiosulfonate (MTSES) and [2-(trimethylammonium)ethyl)]methanethiosulfonate (MTSET). Residue Ile-306(TM5) is close to the verapamil-binding site. It was changed to cysteine, reacted with MTSES or MTSET, and assayed for verapamil-stimulated ATPase activity. Reaction of mutant I306C(TM5) with either compound reduced its affinity for verapamil. We confirmed that the reduced affinity for verapamil was indeed due to introduction of a charge at position 306 by demonstrating that similar effects were observed when Ile-306 was replaced with arginine or glutamic acid. Mutant I306R showed a 50-fold reduction in affinity for verapamil and very little change in the affinity for rhodamine B or colchicine. MTSES or MTSET modification also affected the cross-linking pattern between pairs of cysteines in the drug-binding pocket. For example, both MTSES and MTSET inhibited cross-linking between I306C(TM5) and I868C(TM10). Inhibition was enhanced by ATP hydrolysis. By contrast, cross-linking of cysteine residues located outside the drug-binding pocket (such as G300C(TM5)/F770C(TM8)) was not affected by MTSES or MTSET. These results indicate that the drug-binding pocket is accessible to water.     

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

The Ca(2+)-activated K+ (BK) channel alpha-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 Ca(2+)-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.     

SCAM analysis reveals a discrete region of the pore turret that modulates slow inactivation in Kv1.5

In Kv1.5, protonation of histidine 463 in the S5-P linker (turret) increases the rate of depolarization-induced inactivation and decreases the peak current amplitude. In this study, we examined how amino acid substitutions that altered the physico-chemical properties of the side chain at position 463 affected slow inactivation and then used the substituted cysteine accessibility method (SCAM) to probe the turret region (E456-P468) to determine whether residue 463 was unique in its ability to modulate the macroscopic current. Substitutions at position 463 of small, neutral (H463G and H463A) or large, charged (H463R, H463K, and H463E) side groups accelerated inactivation and induced a dependency of the current amplitude on the external potassium concentration. When cysteine substitutions were made in the distal turret (T462C-P468C), modification with either the positively charged [2-(trimethylammonium)ethyl] methanethiosulfonate bromide (MTSET) or negatively charged sodium (2-sulfonatoethyl) methanethiosulfonate reagent irreversibly inhibited current. This inhibition could be antagonized either by the R487V mutation (homologous to T449V in Shaker) or by raising the external potassium concentration, suggesting that current inhibition by MTS reagents resulted from an enhancement of inactivation. These results imply that protonation of residue 463 does not modulate inactivation solely by an electrostatic interaction with residues near the pore mouth, as proposed by others, and that residue 463 is part of a group of residues within the Kv1.5 turret that can modulate P/C-type inactivation. electrophysiology; voltage-gated potassium channels; substituted cysteine accessibility method     

Charge immobilization caused by modification of internal cysteines in squid Na channels.

We studied the effects of modification of native cysteines present in squid giant axon Na channels with methanethiosulfonates. We find that intracellular, but not extracellular, perfusion of axons with positively charged [(2-trimethylammonium)-ethyl]methanethiosulfonate (MTSET), or 3(triethylammonium)propyl]methanethiosulfonate (MTS-PTrEA) irreversibly reduces sodium ionic (INa) and gating (Ig) currents. The rate of modification of Na channels was dependent on the concentration of the modifying agent and the transmembrane voltage. Hyperpolarized membrane potentials (e.g., -110 mV) protected the channels from modification by MTS-PTrEA. In addition to reducing the amplitudes of INa and Ig, MTS-PTrEA also altered their kinetics such that the remaining INa did not appear to inactivate, whereas Ig was made sharper and declined to baseline more quickly. The shape and amplitude of Ig after modification of channels with MTS-PTrEA appeared to be "charge-immobilized," as if the modified channels were inactivated. MTS-PTrEA did not affect INa or Ig when inactivation was removed by internal perfusion of the axon with pronase. In addition, we find that the steady-state inactivation curve of modified Na channels is made much shallower and is markedly shifted to hyperpolarized potentials. The rates of activation, deactivation, or open-state inactivation were not altered in MTS-PTrEA-modified channels. The uncharged sulfhydryl reagent methymethanethiosulfonate (MMTS) did not affect either INa or Ig, but prevented the irreversible effects of MTS-PTrEA or MTSET on Na channels. It is proposed that the positively charged methanethiosulfonates MTS-PTrEA and MTSET modify a native internal cysteine(s) in squid Na channels, and by doing so promote inactivation from closed states, resulting in charge immobilization and reduction of INa.     

Direct Evidence that Scorpion α-Toxins (Site-3) Modulate Sodium Channel Inactivation by Hindrance of Voltage-Sensor Movements

The position of the voltage-sensing transmembrane segment, S4, in voltage-gated ion channels as a function of voltage remains incompletely elucidated. Site-3 toxins bind primarily to the extracellular loops connecting transmembrane helical segments S1-S2 and S3-S4 in Domain 4 (D4) and S5-S6 in Domain 1 (D1) and slow fast-inactivation of voltage-gated sodium channels. As S4 of the human skeletal muscle voltage-gated sodium channel, hNa_v1.4, moves in response to depolarization from the resting to the inactivated state, two D4S4 reporters (R2C and R3C, Arg1451Cys and Arg1454Cys, respectively) move from internal to external positions as deduced by reactivity to internally or externally applied sulfhydryl group reagents, methane thiosulfonates (MTS). The changes in reporter reactivity, when cycling rapidly between hyperpolarized and depolarized voltages, enabled determination of the positions of the D4 voltage-sensor and of its rate of movement. Scorpion α-toxin binding impedes D4S4 segment movement during inactivation since the modification rates of R3C in hNa_v1.4 with methanethiosulfonate (CH₃SO₂SCH₂CH₂R, where R = -N(CH₃)₃ ⁺ trimethylammonium, MTSET) and benzophenone-4-carboxamidocysteine methanethiosulfonate (BPMTS) were slowed ~10-fold in toxin-modified channels. Based upon the different size, hydrophobicity and charge of the two reagents it is unlikely that the change in reactivity is due to direct or indirect blockage of access of this site to reagent in the presence of toxin (Tx), but rather is the result of inability of this segment to move outward to the normal extent and at the normal rate in the toxin-modified channel. Measurements of availability of R3C to internally applied reagent show decreased access (slower rates of thiol reaction) providing further evidence for encumbered D4S4 movement in the presence of toxins consistent with the assignment of at least part of the toxin binding site to the region of D4S4 region of the voltage-sensor module.     

KCNE peptides differently affect voltage sensor equilibrium and equilibration rates in KCNQ1 K+ channels

KCNQ1 voltage-gated K(+) channels assemble with the family of KCNE type I transmembrane peptides to afford membrane-embedded complexes with diverse channel gating properties. KCNQ1/KCNE1 complexes generate the very slowly activating cardiac I(Ks) current, whereas assembly with KCNE3 produces a constitutively conducting complex involved in K(+) recycling in epithelia. To determine whether these two KCNE peptides influence voltage sensing in KCNQ1 channels, we monitored the position of the S4 voltage sensor in KCNQ1/KCNE complexes using cysteine accessibility experiments. A panel of KCNQ1 S4 cysteine mutants was expressed in Xenopus oocytes, treated with the membrane-impermeant cysteine-specific reagent 2-(trimethylammonium) ethyl methanethiosulfonate (MTSET), and the voltage-dependent accessibility of each mutant was determined. Of these S4 cysteine mutants, three (R228C, G229C, I230C) were modified by MTSET only when KCNQ1 was depolarized. We then employed these state-dependent residues to determine how assembly with KCNE1 and KCNE3 affects KCNQ1 voltage sensor equilibrium and equilibration rates. In the presence of KCNE1, MTSET modification rates for the majority of the cysteine mutants were approximately 10-fold slower, as was recently reported to indicate that the kinetics of the KCNQ1 voltage sensor are slowed by KCNE1 (Nakajo, K., and Y. Kubo. 2007 J. Gen. Physiol. 130:269-281). Since MTS modification rates reflect an amalgam of reagent accessibility, chemical reactivity, and protein conformational changes, we varied the depolarization pulse duration to determine whether KCNE1 slows the equilibration rate of the voltage sensors. Using the state-dependent cysteine mutants, we determined that MTSET modification rates were essentially independent of depolarization pulse duration. These results demonstrate that upon depolarization the voltage sensors reach equilibrium quickly in the presence of KCNE1 and the slow gating of the channel complex is not due to slowly moving voltage sensors. In contrast, all cysteine substitutions in the S4 of KCNQ1/KCNE3 complexes were freely accessible to MTSET independent of voltage, which is consistent with KCNE3 shifting the voltage sensor equilibrium to favor the active state at hyperpolarizing potentials. In total, these results suggest that KCNE peptides differently modulate the voltage sensor in KCNQ1 K(+) channels.     

Accessibility of the CLC-0 Pore to Charged Methanethiosulfonate Reagents

Using the substituted-cysteine-accessibility method, we previously showed that a cysteine residue introduced to the Y512 position of CLC-0 was more rapidly modified by a negatively charged methanethiosulfonate (MTS) reagent, 2-sulfonatoethyl MTS (MTSES), than by the positively charged 2-(trimethylammonium)ethyl MTS (MTSET). This result suggests that a positive intrinsic pore potential attracts the negatively charged MTS molecule. In this study, we further test this hypothesis of a positive pore potential in CLC-0 and find that the preference for the negatively charged MTS is diminished significantly in modifying the substituted cysteine at a deeper pore position, E166. To examine this conundrum, we study the rates of MTS inhibitions of the E166C current and those of the control mutant current from E166A. The results suggest that the inhibition of E166C by intracellularly applied MTS reagents is tainted by the modification of an endogenous cysteine, C229, located at the channel's dimer interface. After this endogenous cysteine is mutated, CLC-0 resumes its preference for selecting MTSES in modifying E166C, reconfirming the idea that the pore of CLC-0 is indeed built with a positive intrinsic potential. These experiments also reveal that MTS modification of C229 can inhibit the current of CLC-0 depending on the amino acid placed at position 166.     

Removal of the outermost arginine in IVS4 segment of the Ca(V)3.1 channel affects amplitude but not voltage dependence of gating current

Positively charged amino acids in S4 segments of voltage-dependent Ca(V)3.1 channel form putative voltage sensor. Previously we have shown that exchange of uppermost positively charged arginine in IVS4 segment for cysteine (mutation R1717C) affected deactivation and inactivation, but not activation of macroscopic current. Now we compared gating currents from both channels. Maximal amplitude of charge movement in R1717C channel decreased but voltage-dependent characteristics of charge movement were not significantly altered. We concluded that mutation of R1717C affects the coupling between S4 activation and pore opening, but not the S4 activation itself.     

State-dependent electrostatic interactions of S4 arginines with E1 in S2 during Kv7.1 activation

The voltage-sensing domain of voltage-gated channels is comprised of four transmembrane helices (S1–S4), with conserved positively charged residues in S4 moving across the membrane in response to changes in transmembrane voltage. Although it has been shown that positive charges in S4 interact with negative countercharges in S2 and S3 to facilitate protein maturation, how these electrostatic interactions participate in channel gating remains unclear. We studied a mutation in Kv7.1 (also known as KCNQ1 or KvLQT1) channels associated with long QT syndrome (E1K in S2) and found that reversal of the charge at E1 eliminates macroscopic current without inhibiting protein trafficking to the membrane. Pairing E1R with individual charge reversal mutations of arginines in S4 (R1–R4) can restore current, demonstrating that R1–R4 interact with E1. After mutating E1 to cysteine, we probed E1C with charged methanethiosulfonate (MTS) reagents. MTS reagents could not modify E1C in the absence of KCNE1. With KCNE1, (2-sulfonatoethyl) MTS (MTSES)⁻ could modify E1C, but [2-(trimethylammonium)ethyl] MTS (MTSET)⁺ could not, confirming the presence of a positively charged environment around E1C that allows approach by MTSES⁻ but repels MTSET⁺. We could change the local electrostatic environment of E1C by making charge reversal and/or neutralization mutations of R1 and R4, such that MTSET⁺ modified these constructs depending on activation states of the voltage sensor. Our results confirm the interaction between E1 and the fourth arginine in S4 (R4) predicted from open-state crystal structures of Kv channels and reveal an E1–R1 interaction in the resting state. Thus, E1 engages in electrostatic interactions with arginines in S4 sequentially during the gating movement of S4. These electrostatic interactions contribute energetically to voltage-dependent gating and are important in setting the limits for S4 movement.     

Conserved residues R420 and Q428 in a cytoplasmic loop of the citrate/malate transporter CimH of Bacillus subtilis are accessible from the external face of the membrane

CimH of Bacillus subtilis is a secondary transporter for citrate and malate that belongs to the 2-hydroxycarboxylate transporter (2HCT) family. Conserved residues R143, R420, and Q428, located in putative cytoplasmic loops and R432, located at the cytoplasmic end of the C-terminal transmembrane segment XI were mutated to Cys to identify residues involved in binding of the substrates. R143C, R420C, and Q428C revealed kinetics similar to those of the wild-type transporter, while the activity of R432C was reduced by at least 2 orders of magnitude. Conservative replacement of R432 with Lys reduced the activity by 1 order of magnitude, by lowering the affinity for the substrate 10-fold. It is concluded that the arginine residue at position 432 in CimH interacts with one of the carboxylate groups of the substrates. Labeling of the R420C and Q428C mutants with thiol reagents inhibited citrate transport activity. Surprisingly, the cysteine residues in the cytoplasmic loops in both R420C and Q428C were accessible to the small, membrane-impermeable, negatively charged MTSES reagent from the external site of the membrane in a substrate protectable manner. The membrane impermeable reagents MTSET,(1) which is positively charged, and AMdiS, which is negatively charged like MTSES but more bulky, did not inhibit R420C and Q428C. It is suggested that the access pathway is optimized for small, negatively charged substrates. Either the cytoplasmic loop containing residues R420 and Q428 is partly protruding to the outside, possibly in a reentrant loop like structure, or alternatively, a water-filled substrate translocation pathway extents to the cytoplasm-membrane interface.     

Molecular Motions of the Outer Ring of Charge of the Sodium Channel: Do They Couple to Slow Inactivation?

In contrast to fast inactivation, the molecular basis of sodium (Na) channel slow inactivation is poorly understood. It has been suggested that structural rearrangements in the outer pore mediate slow inactivation of Na channels similar to C-type inactivation in potassium (K) channels. We probed the role of the outer ring of charge in inactivation gating by paired cysteine mutagenesis in the rat skeletal muscle Na channel (rNav1.4). The outer charged ring residues were substituted with cysteine, paired with cysteine mutants at other positions in the external pore, and coexpressed with rat brain beta1 in Xenopus oocytes. Dithiolthreitol (DTT) markedly increased the current in E403C+E758C double mutant, indicating the spontaneous formation of a disulfide bond and proximity of the alpha carbons of these residues of no more than 7 A. The redox catalyst Cu(II) (1,10-phenanthroline)3 (Cu(phe)3) reduced the peak current of double mutants (E403C+E758C, E403C+D1241C, E403C+D1532C, and D1241C+D1532C) at a rate proportional to the stimulation frequency. Voltage protocols that favored occupancy of slow inactivation states completely prevented Cu(phe)3 modification of outer charged ring paired mutants E403C+E758C, E403C+D1241C, and E403C+D1532C. In contrast, voltage protocols that favored slow inactivation did not prevent Cu(phe)3 modification of other double mutants such as E403C+W756C, E403C+W1239C, and E403C+W1531C. Our data suggest that slow inactivation of the Na channel is associated with a structural rearrangement of the outer ring of charge.     

Gating charges in the activation and inactivation processes of the HERG channel

The hERG channel has a relatively slow activation process but an extremely fast and voltage-sensitive inactivation process. Direct measurement of hERG's gating current (Piper, D.R., A. Varghese, M.C. Sanguinetti, and M. Tristani-Firouzi. 2003. PNAS. 100:10534-10539) reveals two kinetic components of gating charge transfer that may originate from two channel domains. This study is designed to address three questions: (1) which of the six positive charges in hERG's major voltage sensor, S4, are responsible for gating charge transfer during activation, (2) whether a negative charge in the cytoplasmic half of S2 (D466) also contributes to gating charge transfer, and (3) whether S4 serves as the sole voltage sensor for hERG inactivation. We individually mutate S4's positive charges and D466 to cysteine, and examine (a) effects of mutations on the number of equivalent gating charges transferred during activation (z(a)) and inactivation (z(i)), and (b) sidedness and state dependence of accessibility of introduced cysteine side chains to a membrane-impermeable thiol-modifying reagent (MTSET). Neutralizing the outer three positive charges in S4 and D466 in S2 reduces z(a), and cysteine side chains introduced into these positions experience state-dependent changes in MTSET accessibility. On the other hand, neutralizing the inner three positive charges in S4 does not affect z(a). None of the charge mutations affect z(i). We propose that the scheme of gating charge transfer during hERG's activation process is similar to that described for the Shaker channel, although hERG has less gating charge in its S4 than in Shaker. Furthermore, channel domain other than S4 contributes to gating charge involved in hERG's inactivation process.     

The role of the putative inactivation lid in sodium channel gating current immobilization

We investigated the contribution of the putative inactivation lid in voltage-gated sodium channels to gating charge immobilization (i.e., the slow return of gating charge during repolarization) by studying a lid-modified mutant of the human heart sodium channel (hH1a) that had the phenylalanine at position 1485 in the isoleucine, phenylalanine, and methionine (IFM) region of the domain III-IV linker mutated to a cysteine (ICM-hH1a). Residual fast inactivation of ICM-hH1a in fused tsA201 cells was abolished by intracellular perfusion with 2.5 mM 2-(trimethylammonium)ethyl methanethiosulfonate (MTSET). The time constants of gating current relaxations in response to step depolarizations and gating charge-voltage relationships were not different between wild-type hH1a and ICM-hH1a(MTSET). The time constant of the development of charge immobilization assayed at -180 mV after depolarization to 0 mV was similar to the time constant of inactivation of I(Na) at 0 mV for hH1a. By 44 ms, 53% of the gating charge during repolarization returned slowly; i.e., became immobilized. In ICM-hH1a(MTSET), immobilization occurred with a similar time course, although only 31% of gating charge upon repolarization (OFF charge) immobilized. After modification of hH1a and ICM-hH1a(MTSET) with Anthopleurin-A toxin, a site-3 peptide toxin that inhibits movement of the domain IV-S4, charge immobilization did not occur for conditioning durations up to 44 ms. OFF charge for both hH1a and ICM-hH1a(MTSET) modified with Anthopleurin-A toxin were similar in time course and in magnitude to the fast component of OFF charge in ICM-hH1a(MTSET) in control. We conclude that movement of domain IV-S4 is the rate-limiting step during repolarization, and it contributes to charge immobilization regardless of whether the inactivation lid is bound. Taken together with previous reports, these data also suggest that S4 in domain III contributes to charge immobilization only after binding of the inactivation lid.     

Role of Arginine Residues on the S4 Segment of the <Emphasis Type="Italic">Bacillus halodurans</Emphasis> Na<Superscript>+</Superscript> Channel in Voltage-sensing

The one-domain voltage-gated sodium channel of Bacillus halodurans (NaChBac) is composed of six transmembrane segments (S1–S6) comprising a pore-forming region flanked by segments S5 and S6 and a voltage-sensing element composed of segment S4. To investigate the role of the S4 segment in NaChBac channel activation, we used the cysteine mutagenesis approach where the positive charges of single and multiple arginine (R) residues of the S4 segment were replaced by the neutrally charged amino acid cysteine (C). To determine whether it was the arginine residue itself or its positive charge that was involved in channel activation, arginine to lysine (R to K) mutations were constructed. Wild-type (WT) and mutant NaChBac channels were expressed in tsA201 cells and Na⁺ currents were recorded using the whole-cell configuration of the patch-clamp technique. The current/voltage (I-V) and conductance/voltage (G-V) relationships steady-state inactivation (h _∞) and recovery from inactivation were evaluated to determine the effects of the S4 mutations on the biophysical properties of the NaChBac channel. R to C on the S4 segment resulted in a slowing of both activation and inactivation kinetics. Charge neutralization of arginine residues mostly resulted in a shift toward more positive potentials of G-V and h _∞ curves. The G-V curve shifts were associated with a decrease in slope, which may reflect a decrease in the gating charge involved in channel activation. Single neutralization of R114, R117, or R120 by C resulted in a very slow recovery from inactivation. Double neutralization of R111 and R129 confirmed the role of R111 in activation and suggested that R129 is most probably not part of the voltage sensor. Most of the R to K mutants retained WT-like current kinetics but exhibited an intermediate G-V curve, a steady-state inactivation shifted to more hyperpolarized potentials, and intermediate time constants of recovery from inactivation. This indicates that R, at several positions, plays an important role in channel activation. The data are consistent with the notion that the S4 is most probably the voltage sensor of the NaChBac channel and that both positive charges and the nature of the arginine residues are essential for channel activation.This revised version was published online in June 2005 with a corrected cover date.     

GABA(A) receptor M2-M3 loop secondary structure and changes in accessibility during channel gating

The gamma-aminobutyric acid type A (GABA(A)) receptor M2-M3 loop structure and its role in gating were investigated using the substituted cysteine accessibility method. Residues from alpha(1)Arg-273 to alpha(1)Ile-289 were mutated to cysteine, one at a time. MTSET(+) or MTSES(-) reacted with all mutants from alpha(1)R273C to alpha(1)Y281C, except alpha(1)P277C, in the absence and presence of GABA. The MTSET(+) closed-state reaction rate was >1000 liters/mol-s at alpha(1)N274C, alpha(1)S275C, alpha(1)K278C, and alpha(1)Y281C and was <300 liters/mol-s at alpha(1)R273C, alpha(1)L276C, alpha(1)V279C, alpha(1)A280C, and alpha(1)A284C. These two groups of residues lie on opposite sides of an alpha-helix. The fast reacting group lies on a continuation of the M2 segment channel-lining helix face. This suggests that the M2 segment alpha-helix extends about two helical turns beyond alpha(1)N274 (20'), aligned with the extracellular ring of charge. At alpha(1)S275C, alpha(1)V279C, alpha(1)A280C, and alpha(1)A284C the reaction rate was faster in the presence of GABA. The reagents had no functional effect on the mutants from alpha(1)A282C to alpha(1)I289C, except alpha(1)A284C. Access may be sterically hindered possibly by close interaction with the extracellular domain. We suggest that the M2 segment alpha-helix extends beyond the predicted extracellular end of the M2 segment and that gating induces a conformational change in and/or around the N-terminal half of the M2-M3 loop. Implications for coupling ligand-evoked conformational changes in the extracellular domain to channel gating in the membrane-spanning domain are discussed.     

Serotonin and cocaine-sensitive inactivation of human serotonin transporters by methanethiosulfonates targeted to transmembrane domain I

To explore aqueous accessibility and functional contributions of transmembrane domain (TM) 1 in human serotonin transporter (hSERT) proteins, we utilized the largely methanethiosulfonate (MTS) insensitive hSERT C109A mutant and mutated individual residues of hSERT TM1 to Cys followed by tests of MTS inactivation of 5-hydroxytryptamine (5-HT) transport. Residues in TM1 cytoplasmic to Gly-94 were largely unaffected by Cys substitution, whereas the mutation of residues extracellular to Ile-93 variably diminished transport activity. TM1 Cys substitutions displayed differential sensitivity to MTS reagents, with residues more cytoplasmic to Asp-98 being largely insensitive to MTS inactivation. Aminoethylmethanethiosulfonate (MTSEA), [2-(trimethylammonium) ethyl]methanethiosulfonate bromide (MTSET), and sodium (2-sulfonatoethyl)-methanethiosulfonate (MTSES) similarly and profoundly inactivated 5-HT transport by SERT mutants D98C, G100C, W103C, and Y107C. MTSEA uniquely inactivated transport activity of S91C, G94C, Y95C but increased activity at I108C. MTSEA and MTSET, but not MTSES, inactivated transport function at N101C. Notably, 5-HT provided partial to complete protection from MTSET inactivation for D98C, G100C, N101C, and Y107C. Equivalent blockade of MTSET inactivation at N101C was observed with 5-HT at both room temperature and at 4 degrees C, inconsistent with major conformational changes leading to protection. Notably, cocaine also protected MTSET inactivation of G100C and N101C, although MTS incubations with N101C that eliminate 5-HT transport do not preclude cocaine analog binding nor its inhibition by 5-HT. 5-HT modestly enhanced the inactivation by MTSET at I93C and Y95C, whereas cocaine significantly enhanced MTSET sensitivity at Y107C and I108C. In summary, our studies reveal physical differences in TM1 accessibility to externally applied MTS reagents and reveal sites supporting substrate and antagonist modulation of MTS inactivation. Moreover, we identify a limit to accessibility for membrane-impermeant MTS reagents that may reflect aspects of an occluded permeation pathway.     

Control of inward rectifier K channel activity by lipid tethering of cytoplasmic domains

Interactions between nontransmembrane domains and the lipid membrane are proposed to modulate activity of many ion channels. In Kir channels, the so-called "slide-helix" is proposed to interact with the lipid headgroups and control channel gating. We examined this possibility directly in a cell-free system consisting of KirBac1.1 reconstituted into pure lipid vesicles. Cysteine substitution of positively charged slide-helix residues (R49C and K57C) leads to loss of channel activity that is rescued by in situ restoration of charge following modification by MTSET(+) or MTSEA(+), but not MTSES(-) or neutral MMTS. Strikingly, activity is also rescued by modification with long-chain alkyl-MTS reagents. Such reagents are expected to partition into, and hence tether the side chain to, the membrane. Systematic scanning reveals additional slide-helix residues that are activated or inhibited following alkyl-MTS modification. A pattern emerges whereby lipid tethering of the N terminus, or C terminus, of the slide-helix, respectively inhibits, or activates, channel activity. This study establishes a critical role of the slide-helix in Kir channel gating, and directly demonstrates that physical interaction of soluble domains with the membrane can control ion channel activity.