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Department of Physiology, Institute of Hyperexcitability, Jefferson Medical College, Philadelphia, Pennsylvania 19107
Correspondence: Address reprint requests to Dr. Richard Horn, Jefferson Medical College, Dept. of Physiology, Institute of Hyperexcitability, 1020 Locust Street, Philadelphia, PA 19107. Tel.: (215) 503-6725; Fax: (215) 503-2073; E-mail: Richard.Horn{at}TJU.edu
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ABSTRACT |
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-helical structure. Although we obtained an -periodicity index of 2.41 for gating current parameters, a new randomization test produced an indecisive conclusion about the secondary structure of this region. Taken together, our results suggest that the tail end of S6 plays an important role in coupling between activation gating and charge movement. |
INTRODUCTION |
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TOPABSTRACTINTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONACKNOWLEDGEMENTSREFERENCES |
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; Horn, 2000; Sigworth, 1994; Yellen, 1998). We have reasonable candidates for the regions of the channels that subserve these three functions, based on extensive studies, chiefly using mutagenesis and chimeric swapping, and also on the elucidation of the crystal structure of the bacterial potassium channel KcsA (Doyle et al., 1998). Voltage-gated potassium channels, for example, are formed of four subunits, each having six transmembrane segments, S1–S6. The main voltage sensors for this superfamily of ion channels are the four positively charged S4 segments. The four subunits are arranged radially around the pore, which is mainly lined by hydrophobic S6 segments, with selectivity determined by the narrow ‘selectivity filter’ of the extracellular S5–S6 linker (the P-loop). State-dependent modification of cysteine mutants in S6 segments of Shaker potassium channels suggests that the activation gate is located at the cytoplasmic ends of the S6 segments, all four of which converge in a right-handed bundle crossing (Del Camino et al., 2000; Del Camino and Yellen, 2001; Holmgren et al., 1998; Liu et al., 1997).
Extensive data show that S4 segments move in response to changes of membrane potential (Bezanilla, 2000; Horn, 2000; Sigworth, 1994; Yellen, 1998). However, the mechanisms that underlie the coupling between S4 and activation gate movements are unknown. Two hypotheses predominate (see Discussion in Horn, 2000). The first is that S4 movement pulls or twists the cytoplasmic S4–S5 linker, and that this linker is coupled directly or indirectly to the bottom of the S6 segment. The second is that the S4 segment is in contact with the S6 segment within the transmembrane region, so that S4 movement is communicated directly to the S6 segment. Both of these allosteric coupling interactions may contribute to voltage-dependent gating and are not mutually exclusive.
An association between the S4–S5 linker and the bottom of the S6 segment has been proposed to explain the consequences of linker mutations on permeation properties in Shaker potassium channels (Slesinger et al., 1993). A similar association was proposed in studies of chimeric constructs of voltage-gated Shaker potassium channels with KcsA (Lu et al., 2001) and of HERG potassium channels (Tristani-Firouzi et al., 2002). If interaction between the S4–S5 linker and the bottom of S6 contributes to coupling, one would expect that mutations in the cytoplasmic end of S6 would affect charge movement, i.e., the Q–V relationship and/or kinetics of gating current. The S4 segment is also likely to be in direct contact with the S6 segment within the transmembrane region (Durell et al., 1998), allowing S4 conformation to be communicated directly to the S6 segments.
In a previous study, we substituted cysteines for each of eight consecutive residues below the bundle crossing of S6 segments in Shaker potassium channels and found that some cysteine mutants displayed a decrease in open probability and single channel conductance, based on nonstationary noise analysis. Examination of block by tetrabutylammonium indicated that the change of single channel conductance was due to an increase in a local energy barrier to ion movement (Ding and Horn, 2002). Here we examine the effects of these and other S6 tail (S6T) mutants on S4 movement assayed from gating currents, and on activation gate movement assayed from the voltage-dependence and kinetics of ionic currents. Perturbation of the S6T region has consequences on channel activation and especially on gating charge movement, suggesting a role in coupling.
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MATERIALS AND METHODS |
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TOPABSTRACTINTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONACKNOWLEDGEMENTSREFERENCES |
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). In order to increase the expression level, we introduced the Kozak consensus sequence (5'-GCCACCATGG; Kozak, 1991) before the coding region by site-directed mutagenesis. Based on this background, we constructed eight cysteine mutants (N482C, Y483C, F484C, Y485C, H486C, R487C, E488C, and T489C) and their nonconducting versions with the W434F mutation (Perozo et al., 1993) in the pore region. Mutagenesis was done with QuickChangeTM Site-Directed Mutagenesis Kits from Stratagene (La Jolla, CA). All of the cDNA clones were sequenced to verify each mutation. We used a standard calcium phosphate method to transiently transfect tsA201 and HEK293 cells.
Electrophysiology
Standard whole cell patch-clamp recording methods (Ding and Horn, 2001) were used to record gating and ionic currents with an Axopatch 200B amplifier (Axon Instruments, Union City, CA). The patch pipette contained (mM): 105 CsF, 35 NaCl, 10 EGTA, 10 Hepes, pH 7.4. The bath contained (mM): 150 NaCl, 2 KCl, 1.5 CaCl2, 1 MgCl2, 10 Hepes, pH 7.4. All of the experiments were done at room temperature. Liquid junction potentials between the bath and the pipette solution were corrected. Electrode resistance was in the range of 1–2 M 
. The voltage error due to series resistance was <3 mV after compensation. Data were collected between 8–12 min after the establishment of the whole cell configuration in order to avoid time-dependent changes of ionic tail currents and OFF gating currents. For experiments involving cysteine modification by intracellular methanethiosulfonate (MTS) reagents, aqueous stock solutions of 100 mM methanethiosulfonate-ethyltrimethylammonium (MTSET), methanethiosulfonate-ethylsulfonate (MTSES), methanethiosulfonate-2-aminoethyl (MTSEA), and an ethyl acetate stock solution of 100 mM benzophenone-4-carboxylamidocysteine methanethiosulfonate (BPMTS) were kept at 4°C and diluted to 1 mM in the pipette solution immediately before use. Complete modification was achieved within 10 min after the whole cell recording configuration was established. Whole cell and gating currents were low-pass filtered at 5–10 kHz and acquired with a DigiData 1200B digitizer using Clampex 8.0 (Axon Instruments) and sampled at 200 kHz. Capacitance and leakage currents were subtracted by the use of a P/-8 correction protocol from a -120-mV holding potential.
Data analysis
Data were analyzed using pCLAMP (Axon Instruments), ORIGIN 7.0 (OriginLab, Natick, MA), Fortran (Compaq, Houston, TX), and Maple (Waterloo Maple, Ontario, Canada). Throughout the paper, error bars represent the standard error of the mean.
G–V and Q–V relationship
For whole cell current recordings, the voltage-dependence of conductance (G) was estimated from tail currents at -60 mV. Except for the mutant F484C, the contamination of ionic tail currents by OFF gating current at this voltage is negligible. Voltage-dependence of charge (Q) movement was obtained by integration of OFF gating currents from nonconducting mutants at -120 mV. Both G–V and Q–V relations were fitted to the Boltzmann equation:
 | (1) |
Analysis of periodicity
Fourier transform methods (Cornette et al., 1987; Li-Smerin et al., 2000a) were used to evaluate the periodicity of effects of mutations on gating currents. The Gibbs free energy (
G0) was calculated as G0 = qFV1/2, with q and V1/2 determined from Boltzmann fits to Q–V relationships. The change in G0 due to mutation at position j is 
.
The discrete Fourier spectrum P(
) of Gj is defined in terms of angular frequency by
 | (2) |
) and Y() are
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Gj
is the mean value of Gj. The -periodicity index -PI is the average value of P() centered at 105°, relative to the average value of P() in 0°
180°:
 | (3) |
An ideal -helical pattern is characterized by a value of -PI greater than 2 (Cornette et al., 1987; Komiya et al., 1988).
To examine whether the ordered values of Gj in our data could have produced -PI values greater than 2 by chance, we used a randomization test (Lehmann, 1959; Patlak et al., 1986). Such tests have been shown to be most powerful for a large class of alternative hypotheses (Lehmann, 1959). The order of the Gj values was scrambled (i.e., randomized) using a random number generator to produce 1000 artificial datasets, each of which was used to calculate a value of -PI. Note that although there are only eight cysteine mutants, we only examine 1000 out of the 8! = 40,320 possible ordered data sets. The distribution of -PI values for these randomized datasets was compared with the value obtained from the original unscrambled dataset. The original -PI value was considered significant if it was greater than 95% of the values in the randomized datasets. These calculations were done by a Fortran program.
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RESULTS |
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; Horn et al., 2000; Olcese et al., 1997).
Ionic current
Fig. 1 shows whole cell currents in response to families of depolarizations for the wild type channel and each cysteine mutant. Cursory inspection of these currents reveals two notable properties. First, the kinetics of deactivating tail currents vary considerably for individual mutants, slowest for N482C and fastest for F484C1. Note that we measured these tail currents at a relatively depolarized voltage of -60 mV to avoid contamination by OFF gating currents, which have very small amplitudes except at more hyperpolarized voltages (e.g., Fig. 2). Second, the relative amplitudes of peak ionic and gating current at depolarized voltages differ among the mutants. At +60 mV, the peak ionic current is 3.8 times larger than the peak gating current for wild type channels. By contrast, the peak gating current for the F484C mutant is 3 times larger than the ionic current at +60 mV. The ionic current is also relatively small in the Y485C mutant. The relatively small ionic currents in these two mutants are probably due to reductions of open probability and/or single channel conductance (Ding and Horn, 2002). We previously reported that F484C had both a decreased single channel conductance and a low open probability, while Y485C had only a decreased single channel conductance.
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). The ON gating current of each mutant increased in peak amplitude and rate of decay with increased depolarization. The OFF gating current is fast and without obvious rising phase after a small depolarization, and except for the mutants F484C and Y485C, OFF gating currents exhibit a quick decay followed by a slower one after intermediate depolarizations. Following depolarizations to voltages larger than -30 mV, the OFF gating currents show a pronounced rising phase followed by a slow decay. The initial fast outward spike present in OFF gating currents, following a large depolarization in some cells, is likely due to contamination by nonlinear capacity currents during our capacitance correction procedure (Stühmer et al., 1991). The kinetics of ON gating currents in response to a series of depolarizations are rather comparable for all mutants, with decay time constants differing by less than a factor of two (Fig. 3 A). This suggests that early transitions along the activation pathway, primarily involving the independent movement of individual S4 segments (Bezanilla et al., 1994; Horn et al., 2000; Schoppa and Sigworth, 1998; Smith-Maxwell et al., 1998), are relatively insensitive to these mutations. By contrast, the OFF gating currents at -120 mV show a more pronounced mutation-dependent slow decay phase after depolarizations to voltages above about -30 mV (Fig. 2 and Fig. 3, B and C). N482C and F484C have the slowest and fastest OFF kinetics, respectively, the difference between them being larger than 10-fold. The channel constructs studied show a positive correlation between OFF gating current kinetics and decay kinetics of ionic tail currents at -120 mV (Fig. 3 D). This correlation is consistent with the coupling between voltage sensors and the activation gate for late transitions in the activation pathway, especially an open-to-closed transition. Although the correlation shown depends largely on the gating parameters from two mutants, N482C and Y485C, this relationship would be further strengthened if we could have included data from the F484C mutant, which has both the fastest deactivation kinetics and OFF gating current kinetics of all the constructs examined. However the ionic tail currents were too fast to be measured accurately.
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20 mV among the mutants. The mutant F484C has the largest effect on the Q–V relationship, both on the slope (a 52% increase), and on the midpoint (an 11.4 mV hyperpolarizing shift compared to wild type channel). Another interesting characteristic of the F484C mutant is that it has a left-shifted Q–V curve (Fig. 4), but a right-shifted G–V curve (Fig. 2 in Ding and Horn, 2001), suggesting that this mutation uncouples the movements of the voltage sensor and the activation gate.
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). In order to test its sensitivity to structural perturbation, we substituted different amino acids at position 484 and measured Q–V and OFF gating current decay. Fig. 5 A shows the gating currents of WT and five mutant channels at position 484. The midpoints of Q–V relations vary over a range of 15 mV (Fig. 5 B). In general, residues with a bulky aromatic side chain have slower OFF gating currents after large depolarizations, compared to those with relatively small side chains (Fig. 5 B). This suggests that an aromatic side chain is important to maintain normal charge return from the open state. This conclusion is further validated by modifying F484C with methanethiosulfonate reagents. When F484C is modified by BPMTS, which attaches a benzophenone moiety with two benzene rings to the cysteine, the OFF gating current decay becomes slow, similar to the WT, after large depolarizations (Fig. 5 C). However, when F484C is modified with the smaller hydrophilic reagents MTSEA, MTSET, and MTSES, there is little effect on the OFF gating current decay (Figs. 5 C and 6 A).
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), consistent with a destabilized open state. This could be a consequence of a faster open
closed rate, which reasonably would correlate with faster kinetics of OFF gating currents. The results of Fig. 6 show that constructs in which 484 residues have small non-aromatic side chains expedite closing rates.
Analysis of periodicity
Shifts of the Q–V relationships (Table 1) for successive cysteine mutants show a periodicity that may give some insight into the secondary structure of the S6T region. To explore these features, we subjected the fitted parameters of these Q–V relationships to a Fourier analysis of periodicity (see Methods) after converting the data into free energy differences from wild type values (Fig. 7 A). Fig. 7 B shows the discrete power spectrum for the Q–V shifts which has a major peak centered at 108°. This spectrum is suggestive of an amphipathic -helix, which is expected to produce a peak near 100°, the angle subtended by successive side chains in a canonical -helix. The periodicity index, -PI, is used to provide an objective criterion of helicity. -PI values >2 are considered evidence of an -helical structure (Cornette et al., 1987; Komiya et al., 1988). The spectrum in Fig. 7 B has an -PI value of 2.41, suggesting that this short stretch of residues has an -helical structure.
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-PI value is >2, we were concerned that the apparent periodicity might be a chance occurrence due to the small number of residues (eight) in our study. To investigate this possibility we employed a nonparametric statistical procedure known as a randomization test (see Methods). We wanted to test whether the high -PI values we obtained could have occurred by the chance ordering of the measured Gj values for these cysteine mutants. We therefore created 1000 datasets, each of which contained the original eight Gj values, but in randomized order. We calculated the -PI values for each of these datasets and compared the distribution of -PIs in the randomized datasets to that obtained from the original ordered dataset. The distribution is shown in Fig. 7 C with an arrow designating the original -PI value. For the Q–V measurement, 72 of the 1000 -PI values were greater than -PI of the original dataset. Therefore, although the original -PI values of the spectrum shown in Fig. 7 B is >2, this may have occurred by chance (P 
0.072). Therefore, the -helicity of the S6T region remains unsettled. |
DISCUSSION |
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). Here we further report that the S6T region influences activation gating and charge movement. The main effects of S6T mutations are Q–V shifts and changes in the time constants of ionic tail currents and OFF gating currents. The positive correlation between these latter two kinetic parameters is consistent with the typically strong coupling between activation gating and charge movement (Sigg and Bezanilla, 1997; Sigworth, 1994). The residue that is most sensitive to cysteine substitution is F484. Our results suggest that an aromatic side chain at this position is critical for its normal contribution to gating. Finally, a spectral analysis of the effects of cysteine mutants shows evidence for -helical periodicity, although a randomization test does not lead to a high level of confidence in this conclusion.
The two aromatic residues in S6T, F484 and Y485, are highly conserved among KV channels. Y485 is absolutely conserved, whereas F484 is only substituted by tyrosine or isoleucine (Liu et al., 1997). Cysteine mutations of F484 and Y485 cause: 1. an increase in the rate of deactivation of ionic currents, 2. an increase in the rate of charge return seen in OFF gating currents, 3. a small, but significant, decrease in the time constant for ON gating currents, and 4. a hyperpolarizing shift of the Q–V curve for F484C. Many of these effects can be described as a partial uncoupling of the conformation of the voltage sensor from that of the activation gate due to the structural perturbation caused by mutagenesis. Our results suggest, for example, that normal voltage sensor movement is impeded by coupling to the activation gate. Therefore, uncoupling can allow more rapid kinetics of charge movement in many of the mutants. This is especially manifest in transitions near the open state in the activation pathway, accounting for larger effects on OFF than ON gating current. Partially disrupted coupling in these mutants is also suggested by decreases in Po,max (Ding and Horn, 2002) and by hyperpolarizing shifts of Q–V curves in some constructs, as if unloading S6T from the S4–S5 linker allows the S4 segment to carry its positive charge outward more easily when depolarized.
The S6T region is just downstream from the activation gate formed by the bundle crossing of the channel's four S6 segments. Allosteric effects on the kinetics of ionic tail currents are not, therefore, difficult to rationalize, because conformational changes in this region are likely to accompany the opening and closing of the activation gate. But how does the S6T region affect the S4 movement that underlies gating current? We consider three possibilities. The first possibility is that S6T mutations produce global disruptions of structure that affect all biophysical properties of the channel. This possibility cannot be eliminated, although the consequences of these mutations are generally rather mild on gating and have little effect on the selectivity of the pore (Ding and Horn, 2002). The second possibility is that the cytoplasmic S6T region has direct interaction with the S4–S5 linker, as proposed previously (Horn, 2000; Lu et al., 2001; Tristani-Firouzi et al., 2002). Therefore, mutations in S6T might affect S4 movement due to conformational coupling between these cytoplasmic regions. Finally, mutations of S6T might produce upstream allosteric consequences on the S6 segment in its transmembrane region, where it is likely to directly contact the S4 segment (Durell et al., 1998).
Circumstantial evidence provides support for the last two of the above three possibilities—either a cytoplasmic contact between S6T and the S4–S5 linker, or a transmembrane interaction between the S4 and S6 segments. For example, as in the S6T region, mutations in the S4–S5 linker affect permeation, activation gating, and charge movement (Isacoff et al., 1991; McCormack et al., 1991; Sanguinetti and Xu, 1999; Schoppa et al., 1992; Slesinger et al., 1993; Tristani-Firouzi et al., 2002); however, the relative magnitudes of effects on these gating processes differs between S6T and the S4–S5 linker. Our results using S6T mutations show somewhat larger effects on charge movement than on activation gating (Fig. 4), whereas mutations of some S4–S5 residues produce dramatic effects on activation (shifts of >70 mV of G–V curves) with only minor consequences on charge movement (Schoppa et al., 1992). Although the collected results could be explained by a direct interaction between these cytoplasmic regions, this hypothesis remains speculative. Two studies, however, show the possibility of electrostatic interactions between specific residues in these two regions, one examining sodium channels (Smith and Goldin, 1997), the other the HERG potassium channel (Tristani-Firouzi et al., 2002). Our periodicity analysis suggests that the S6T region might have an -helical structure. The S4–S5 linker has also been proposed to have an -helical secondary structure (Duclohier et al., 1997; Ohlenschläger et al., 2002). It is tempting, therefore, to speculate that S6T and the S4–S5 loop form a helix bundle with a critical role in coupling charge movement and activation gating, although direct evidence is lacking.
Other studies suggest that interactions between S4 and S6 segments occur in the transmembrane region. For example, tryptophan scanning mutagenesis of the S6 segment of Shaker produces effects on ionic currents that could be explained by an interaction of the backside of the S6 helix (directed away from the central axis of the pore) with the S4 segment (Li-Smerin et al., 2000b). Mutagenesis above the S6 bundle crossing also affects gating currents (Ding et al., 2002; Hackos et al., 2002). Some of these effects could be due to direct interactions between S4 and S6 segments.
A ‘kink’ or ‘bend’ in the S6 segment is likely to direct the bottom part of S6 outward toward the S4 segment (Del Camino et al., 2000; Del Camino and Yellen, 2001), especially when the channel is open (Jiang et al., 2002a; Jiang et al., 2002b). One motivation for the suggestion of a kink is the presence of a conserved Pro-X-Pro sequence near the bottom of the S6 segments of all KV channels. However, other voltage-gated potassium channels lack the Pro-X-Pro sequence to serve as inflection points for the postulated kink in Shaker. For example, calcium-activated potassium channels that are also voltage-dependent have a single proline near the bottom of S6 (Pallanck and Ganetzky, 1994), whereas the S6 segment of HERG potassium channels has no prolines (Warmke and Ganetzky, 1994). Likewise, the voltage-dependent Shaker-KcsA chimera (Lu et al., 2001) lacks prolines in its S6 segments. The crystal structure of the open MthK potassium channel suggests the presence of another kink, centered on a glycine residue that is seven residues upstream of Shaker's Pro-X-Pro sequence (Jiang et al., 2002a; Jiang et al., 2002b). This kink also directs the bottoms of the four S6 segments outward toward other transmembrane segments when the channel is open.
A pivotal role for the S6T region in the coupling of gate opening with an activating stimulus is suggested by our understanding of structurally related ion channels, specifically cyclic nucleotide gated (CNG) and eukaryotic calcium-activated potassium channels. In both of these types of channels, cytoplasmic agonists bind with the C-terminal extensions of the S6T regions of individual subunits, causing opening of the activation gate. One can easily imagine that conformational changes induced by these binding events are communicated directly to the S6T regions and from there to the transmembrane S6 segments, as proposed for homologous regions of a bacterial potassium channel (Jiang et al., 2002b). Detailed studies of the S6 and S6T regions of eukaryotic calcium-activated potassium channels remain to be undertaken. However some information is available for CNG channels, where agonist binding appears to cause a rotation of both the S6 segments and the S6T regions, and a concomitant widening of the opening at the bundle crossing (Eaholtz and Zagotta, 2001; Johnson and Zagotta, 2001). By contrast with the model of del Camino et al. (2000) for Shaker, in which S6T regions diverge from the central axis of the pore, the four S6T regions of CNG channel subunits are postulated to converge below the bundle crossing (Johnson and Zagotta, 2001). This convergence is also proposed for the cytoplasmic extensions of the inner helices of KcsA channels (Cortes et al., 2001). Although an interaction between S6T and the bottom of the S4 segment makes teleological sense for a voltage-gated channel, there is no obvious reason for the S6T regions of CNG channels, which are not voltage-dependent, to be oriented toward the membrane where they might be able to interact with the S4–S5 linker.
The results of this and a previous study (Ding and Horn, 2002) reveal functional roles for the S6T region of Shaker potassium channels. Permeation, activation gating, and charge movement are all affected by S6T mutations. Future studies will elucidate whether this region plays an essential role in coupling these biophysical properties.
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ACKNOWLEDGEMENTS |
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Supported by Grant AR41691 to R.H. from the National Institutes of Health.
Submitted on August 5, 2002; accepted for publication September 20, 2002.
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REFERENCES |
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on(V) = exp(-qonV/kT). The partial charge values qon were 0.49, 0.39, 0.29, 0.29, 0.33, 0.41, 0.38, 0.39, and 0.45eo for WT, N482C, Y483C, F484C, Y485C, H486C, R487C, E488C, and T489C, respectively. (B) OFF gating current decay time constants at -120 mV plotted against the activating voltage. Following either very hyperpolarized or large depolarized voltage steps, the decay of OFF gating currents can generally be fitted by a single exponential function. As a rough approximation, we also fit the decay of OFF gating currents following intermediate voltage steps with a single exponential. (C) OFF time constants at -120 mV following a step to +40 mV. (D) Correlation between deactivation time constants of ionic currents (-120 mV) and gating current time constants (-120 mV) after depolarizations to +40 mV. Data from 3
