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Department of Physiology, University of Pennsylvania School of Medicine, Philadelphia, PA 19104

Correspondence to Frank T. Horrigan: Horrigan{at}mail.med.upenn.edu

TOP ABSTRACT INTRODUCTION MATERIALS AND METHODS RESULTS DISCUSSION REFERENCES

 
The activation of large conductance Ca²⁺-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 ((I_K)) over an extended voltage range in 0–50 µM [Ca²⁺]_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 (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.

X.J. Lou's present address is Johnson & Johnson Pharmaceutical Research and Development, Spring House, PA 19477.

	INTRODUCTION

TOP ABSTRACT INTRODUCTION MATERIALS AND METHODS RESULTS DISCUSSION REFERENCES

 
To sense voltage, ion channels must contain charged residues whose position in the membrane electric field change upon voltage sensor activation. Identifying these residues and their contributions to voltage sensitivity are critical to understanding the gating of any voltage-dependent channel. Voltage-dependent K⁺ channels share a common "core" architecture, including six transmembrane segments (S1–S6) with an S1–S4 voltage sensor and S5–S6 pore domain in each subunit (Fig. 1 A). Many conserved basic and acidic amino acids are present in S1–S4 that could potentially contribute to voltage sensing (Fig. 1 B). However, in Shaker, only four residues in S4 and one in S2 account for the majority of gating charge (Fig. 1 B, double starred positions) (Aggarwal and MacKinnon, 1996; Seoh et al., 1996). That a few charged residues make large contributions to voltage sensitivity is supported by evidence in Shaker (Larsson et al., 1996; Starace and Bezanilla, 2001), hERG (Zhang et al., 2004), and Na⁺ channels (Yang et al., 1996) that the accessibility of S4 positions to internal and external solutions can switch sides upon voltage sensor activation, implying that some charges traverse the entire electric field. Although the majority of charged residues in S1–S4 appear to be non–voltage sensing, their conservation suggests they also play important roles in channel structure or function. Salt bridge interactions between oppositely charged amino acid side chains in different transmembrane segments, including non–voltage-sensing residues, are observed in the crystal structures of KvAP (Jiang et al., 2003) and Kv1.2 (Long et al., 2005a), and impact Shaker biogenesis (Papazian et al., 1995; Tiwari-Woodruff et al., 1997). Non–voltage-sensing residues also influence channel gating, suggesting they participate in interactions that depend on the activation state of the voltage sensor (Tiwari-Woodruff et al., 2000).

View larger version (47K): [in this window] [in a new window]   Figure 1. Charged residues in the transmembrane segments of BK and KV channels. (A) The membrane topology of Slo1 and Shaker potassium channel subunits. Both contain a core domain including S1–S4 voltage sensor and S5–S6 pore. Slo1 contains an additional NH2-terminal transmembrane segment (S0) and large COOH-terminal tail. Conserved basic (+) and acidic (–) amino acids in the S1–S4 segments are indicated. (B) Multiple sequence alignment of voltage sensor domain from mouse and Drosophila homologues of Slo1 (mSlo1, dSlo1) and KV channels (KVAP2.1, KVAP, Shaker, KV1.2) based on Jiang et al. (2003). Putative transmembrane segments are denoted by solid lines based on hydropathy analysis of Slo1 (Wallner et al., 1996) and dashed lines based on the structure of KVAP (Jiang et al., 2003). Charged residues that are highly conserved in Slo1 or in KV channels are bold. Positions that were mutated in mSlo1 are numbered and indicated by boxes. Potential voltage-sensing residues in Shaker are indicated by stars, with double stars indicating those where mutation has the greatest impact on gating charge (Aggarwal and MacKinnon, 1996; Seoh et al., 1996).

Several mechanisms could account for the relatively weak voltage dependence of BK channel activation. First, voltage sensor movement in Slo1 may be limited compared with Shaker, such that the number of voltage-sensing positions is reduced and/or each residue makes a smaller contribution to gating charge. A reduced contribution of individual residues seems likely, since even one S4 arginine traversing the entire electric field, as in Shaker, should exceed the total gating charge of mSlo1. Alternatively, S4 residues could make large contributions to gating charge if additional sites make contributions of opposite polarity such that the net gating charge is small. Finally, fundamental differences in the structure and/or movement of voltage sensors in BK and K_V channels may exist, such that voltage-sensing residues in Slo1 correspond to non–voltage-sensing positions in Shaker, and the pattern of charge residues is not predictive of differences in voltage sensitivity.

Here we examine the effects on voltage-dependent activation of mutating each charged residue in the S1–S4 segments of mSlo1 to understand their role in channel function, to identify voltage-sensing residues, and to determine why BK channels are weakly voltage dependent. Our results indicate that while many charged residues influenced BK channel gating, only four are potentially voltage sensing, and only one is in S4. Charge neutralization at any of these sites reduces voltage sensitivity but the decreases in gating charge are small (0.3 e per subunit). The limited contribution of S4 suggests that voltage sensor movement in BK channels is reduced relative to K_V channels and indicates that charged residues outside of S4 make significant contributions to gating charge. That potential voltage-sensing residues in S2 are not in the same location for mSlo1 and Shaker suggests that additional differences exist in the movement or conformation of voltage sensors in these channels. Thus several factors may contribute to the weak voltage dependence of BK channel activation. In addition, our results show that non–voltage-sensing residues make important contributions to voltage gating, in some cases influencing the energetic coupling of voltage sensor activation to channel opening, in others profoundly influencing the equilibrium constant for voltage sensor activation.

	MATERIALS AND METHODS

TOP ABSTRACT INTRODUCTION MATERIALS AND METHODS RESULTS DISCUSSION REFERENCES

 
Channel Expression
Experiments were performed with the mbr5 clone of the mouse homologue of the Slo1 gene (mSlo1) (Butler et al., 1993) expressed in Xenopus oocytes. The clone was modified to facilitate mutagenesis and was propagated and cRNA transcribed as described previously (Cox et al., 1997). Oocytes were injected with 0.5–50 ng of cRNA, incubated at 18°C, and studied 3–7 d after injection. Site-directed mutagenesis was performed with the QuikChange XL Site-Directed Mutagenesis Kit (Stratagene) and confirmed by sequencing. Some mutants (E180A, D186A, R210N, and E219Q) were provided by J. Cui (Washington University, St Louis, MO).

Electrophysiology and Data Analysis
Currents were recorded using the patch clamp technique in the inside-out or outside-out configuration (Hamill et al., 1981). For I_K measurements, the internal solution contained (in mM) 110 K-methanesulfonic acid (K-MES), 20 HEPES. 40 µM (+)-18-crown-6-tetracarboxylic acid (18C6TA) was added to chelate contaminant Ba²⁺ (Diaz et al., 1996; Neyton, 1996). In addition, "0 Ca²⁺" solution contained 5 mM EGTA, reducing free Ca²⁺ to an estimated 0.8 nM in the presence of 10 µM contaminant Ca²⁺. Solutions containing Ca²⁺ were buffered with 5 mM HEDTA, and free [Ca²⁺] was measured with a Ca²⁺ electrode (Orion Research Inc.). Nominal [Ca²⁺] reported as 1, 10, and 50 µM corresponded to measured concentrations of 0.87, 8.7, and 49.9 µM, respectively. Ca²⁺ was added as CaCl₂, and [Cl^–] was adjusted to 10 mM with HCl. The external solution contained 110 K-MES, 2 MgCl₂, 6 HCl, 20 HEPES. For gating current measurements, the internal solution contained 135 NMDG-MES, 6 NMDG-Cl, 20 HEPES, 2 EGTA, 40 µM 18C6TA. The external solution contained 125 TEA-MES, 2 TEA-Cl, 2 MgCl₂, 20 HEPES. The pH of all solutions was adjusted to 7.2 with MES. Experiments were performed at room temperature (20–22°C).

Data were acquired with an Axopatch 200B amplifier (Axon Instruments, Inc.) in patch mode with the Axopatch's filter set at 100 kHz. Currents were subsequently filtered by an 8-pole Bessel filter (Frequency Device, Inc.) at 20 kHz and sampled at 100 kHz with an 18-bit A/D converter (Instrutech ITC-18). A P/4 protocol was used for leak subtraction (Armstrong and Bezanilla, 1974) with a holding potential of –80 mV. For some mutants, with increased P_O, current traces in high [Ca²⁺] were leak subtracted using a leak trace recorded in 0 Ca²⁺ at V –140 mV before and after changing [Ca²⁺]_i. Electrodes were made from thick-walled 1010 glass (World Precision Instruments, Inc.) and their tips coated with wax (KERR Sticky Wax). The electrode's resistance in the bath solution (1.0–2.5 M) was used as an estimate of series of resistance (R_S) for correcting the voltage at which macroscopic I_K was recorded. Series resistance error was <15 mV for all data presented. A Macintosh-based computer system was used in combination with Pulse Control acquisition software (Herrington and Bookman, 1995) and Igor Pro for graphing and data analysis (WaveMetrics, Inc.). A Levenberg-Marquardt algorithm was used to perform nonlinear least-squared fits.

Open probability (P_O) was estimated over a wide voltage range by recording macroscopic I_K when P_O was high (0.005–0.05), and single channel currents in the same patch when P_O was low (0.01–0.1). Macroscopic conductance (G_K) was determined from tail currents at –80 mV, following 30-ms voltage pulses, and was normalized by G_Kmax measured in 50 µM Ca²⁺ to estimate P_O. At more negative voltages, NP_O was determined from steady-state recordings of 1–60 s duration that were digitally filtered at 5 kHz. NP_O was determined from all-points amplitude histograms by measuring the fraction of time spent (P_K) at each open level (K) using a half-amplitude criteria and summing their contributions. . P_o was then determined by estimating N from G_Kmax in 50 µM Ca²⁺ (N = G_Kmax/g_K, where g_K is the single channel conductance at –80 mV).

Patch to patch variation in the half-activation voltage (V_h) of the G_K-V relationship is observed for Slo1 channels (Stefani et al., 1997; Horrigan et al., 1999) and causes broadening in the averaged voltage-dependent relationships relative to individual experiments. To compensate for such variation, V_h was determined for each patch and P_o-V relations were shifted along the voltage axis by V_h = (V_h – V_h), where V_h is the mean for all experiments at the same [Ca²⁺], before averaging (Horrigan and Aldrich, 1999; Horrigan et al., 1999).

Mean activation charge displacement (q_a = kT d(ln(P_O)/dV)) was measured from the slope of the ln(P_O)-V relation by linear regression over 60-mV intervals (approximately four data points) and plotted against mean voltage. This procedure minimized noise while introducing errors of at most 5% in q_a, based on simulations using the HCA model (Horrigan et al., 1999). Fits of the q_a-V relation by gating schemes were similarly determined by simulating the data at 20-mV intervals and determining q_a by linear regression.

Gating currents were measured using admittance analysis as previously described (Horrigan and Aldrich, 1999). In brief, inside-out patches were excised into nominally K⁺-free solutions containing isotonic TEA in the extracellular solution to block residual ionic currents. Currents were recorded in response to 0.5–1-s voltage ramps upon which a sinusoidal voltage command (1736 hz, 60 mV peak to peak) was superimposed. Admittance was calculated for each cycle of the sinwave, and capacitance was determined after correcting for phase shifts due to instrumentation. The voltage-dependent component of the capacitance signal due to gating current was integrated over the voltage range to determine the Q-V relation, which was sampled and plotted at 20-mV intervals. The resulting Q-V is a pseudo steady-state measurement that approximates the closed channel charge distribution (Q_C) at voltages where P_O is small (Horrigan and Aldrich, 1999).

The steady-state data in 0 Ca²⁺ were fit with the HCA model using a semi-automated procedure to estimate the best values and standard deviation for each parameter based on least-squares criteria. After determining the best fit to the log(P_o)-V relation, with all parameters allowed to vary, the parameters were refined by iteratively fitting q_a-V and log(P_O)-V. First the voltage sensor charge (z_J) was varied to fit q_a at voltages where P_O < 0.1. Under these conditions, q_a is highly dependent on z_J. Log(P_O)-V was then fit with all parameters except z_J allowed to vary. The procedure was repeated until z_J approached a constant value. In this way, reasonable fits were obtained to both log(P_O) and q_a, and the values of charge (z_J) and coupling (D) were better constrained than by fitting either relation alone. In some cases where gating was shifted to very negative or positive voltages (R207Q,E; R210C; R213C,E; and D153C,K), the coupling factor D was poorly constrained and was held to the wild-type (WT) value until z_J was determined; and then D was allowed to vary with z_J held constant. Data in multiple [Ca²⁺] were fit by eye using the HA model (see RESULTS).

	RESULTS

TOP ABSTRACT INTRODUCTION MATERIALS AND METHODS RESULTS DISCUSSION REFERENCES

 
Mutation of Charged Residues in S1–S4 Alter mSlo1 Gating
To study the role of charged residues in the BK channel voltage sensor, we examined the effects on the voltage dependence of steady-state activation (P_O) and macroscopic kinetics ((I_K)) of mutating individual sites in the S1, S2, S3, and S4 segments of mSlo1 indicated in Fig. 1 B. Charged residues were replaced by neutral (A, C, N, Q) or charged (E, K) amino acids to determine the effects of reducing or reversing charge. In addition, a neutral residue in S2 (Y163) was replaced by Glu (E), to match a voltage-sensing position in Shaker (E293). I_K was recorded over a wide voltage range in the virtual absence of internal Ca²⁺ (0 Ca²⁺, see MATERIALS AND METHODS) to isolate effects of mutation on voltage-dependent gating from those on Ca²⁺-dependent mechanisms or the closed to open conformation change (Horrigan and Aldrich, 2002). Measurements were also performed in various [Ca²⁺]_i, including a nearly saturating concentration (50 µM) used to determine the maximal conductance (G_Kmax) and estimate the number of channels (N) in each patch to determine P_o (see MATERIALS AND METHODS).

Charge-altering mutations at all sites tested produced functional channels that express macroscopic currents in excised patches. In response to voltage pulses, currents recorded in 0 Ca²⁺ or 50 µM Ca²⁺ activate and deactivate with an approximately exponential time course, qualitatively similar to the WT channel (Fig. 2, A–C). However most mutations in S2, S3, and S4 altered channel gating significantly, as shown in Fig. 2 D by comparing normalized G_K-V relations for WT and mutant channels in 0 Ca²⁺. Although R207Q, R207E, or R210C in S4 increased P_O relative to the WT and shifted G-V curves to more negative voltages, most mutations inhibited activation. Indeed some mutants appeared almost nonfunctional in 0 Ca²⁺, but we were able to characterize their gating properties owing to the high single channel conductance and Ca²⁺ sensitivity of BK channels. For instance, a voltage pulse to +180 mV in 0 Ca²⁺ evoked only single channel currents from a patch expressing R213C channels (Fig. 2 C, left), whereas macroscopic currents are evoked from the same patch in 50 µM Ca²⁺ (Fig. 2 C, right). This shows that hundreds of channels are present and functional, and that P_O in 0 Ca²⁺ is low but measurable based on the resolution of discrete opening events.

View larger version (50K): [in this window] [in a new window]   Figure 2. Mutation of charged residues in voltage sensor domain alter mSlo1 gating. Families of IK evoked from (A) WT (B) R207Q, and (C) R213C channels in response to pulses to different voltages at 20-mV intervals from a holding potential of –80 mV. Currents in 0 Ca2+ and 50 µM Ca2+ for each channel were recorded from the same patch. Dashed lines indicate the zero current level. (D) GK-V relations (mean ± SEM) for WT and mutant channels are normalized by GKmax determined in 50 µM Ca2+ and are fit by Boltzmann functions (lines). WT (•), R113Q (), D133Q (), D153K (), D153C (), Y163E (), R167E (), R167A (), E180A (), D186A (), R201Q (), R207E (), R207Q (), R210C (), R210E (), R210N (), R213C (), R213E (), E219Q ().

View larger version (39K): [in this window] [in a new window]   Figure 3. Data analysis and modeling. (A) Po-V relation for WT mSlo1 channels in 0 Ca2+ (mean ± SEM) is plotted on a semilog scale and fit by the HCA model (solid line, see be-low). The limiting slope at negative voltages is indicated by a dashed line representing the partial charge associated with channel opening (zL = 0.3 e). (B) qa-V relation determined from the logarithmic slope of mean PO (see MATERIALS AND METHODS). (C) HCA gating mechanism asserts that equilibration of the channel gate between closed and open (C–O) is influenced allosterically by four independent and identical voltage sensors that each can be in a resting or activated state (R–A). The equilibrium constants for channel opening L and voltage sensor activation J are voltage dependent with partial charges zL and zJ, respectively (). The activation of each voltage sensor increases the C–O equilibrium constant by an allosteric coupling factor D. (D) Gating scheme shows the closed and open states (Ci, Oi, where i = number of activated voltage sensors) and equilibrium constants specified by the HCA mechanism. Horizontal transitions represent voltage sensor activation, and vertical transitions represent channel opening. Solid lines in A and B represent best fits to the HCA model (zJ = 0.59 e, zL = 0.3 e, J0 = 0.017, Lo = 1.4 x 10–6, D = 23.1) determined by a semi-automated method (see MATERIALS AND METHODS). Dashed lines in B indicate the charge distribution for open channels (QO, Eq. 5) and the difference between charge distributions for open and closed channels Qo – Qc, Eq. 6), defined by the fit parameters. (E–H) Predicted effects of changing various parameters in the HCA model. (E) Changes in peak qa, expressed as a fraction of the control value (fqaMAX), produced by changing gating charge (zJ, zL) are directly proportional to the fractional change in total gating charge (fzT, where zT = zL + 4zJ). Dashed line indicates unity slope (b = 1). Solid lines indicate effects of proportional changes in both zL and zJ (b = 0.99) or changing zJ alone (b = 0.94). (F) Effects on fqaMAX of fractional changes in L0, J0, or D. (G) Effects on PO-V relation of changing zJ(0.35 e), D(5.1), J0(1.7), or L0(1.4 x 10–4) and leaving other parameters the same as the WT (solid line). (H) The decreases in zJ or D both decrease qaMAX relative to the WT (solid line) but have distinct effects on the qa-V relations. In particular, the steepness of the foot of the curve is reduced together with zJ but is not altered by changing D.

View larger version (46K): [in this window] [in a new window]   Figure 4. Effects of voltage sensor mutations on gating charge and allosteric coupling. (A) qaMAX for each voltage sensor mutant was determined from the mean PO-V relation in 0 Ca2+ (see MATERIALS AND METHODS) and normalized to that of the WT (1.89 e). qaMAX for R210C could not be determined for reasons discussed in the text. (B) The total gating charge (zT = zL + 4zJ) and (C) allosteric coupling factor D were estimated from fits of PO-V and qa-V relations to the allosteric models and normalized to those for the WT (zT = 2.62 e, D = 23.9). Shaded bars were determined by semi-automated fitting of the HCA model to 0 Ca2+ data (see MATERIALS AND METHODS). Solid bars represent fits to data in all [Ca2+] using the HA model (Table I) with parameters adjusted manually. (D and E) Confidence limits for manual fits were estimated for zT or D by adjusting zJ (panel D) or D (panel E) respectively from the best fit values (solid line) to exceed the error range of PO as indicated by dashed lines.

(1)

For channels that open only when all voltage sensors are activated, q_a increases at negative voltages approaching a maximum or limiting slope (q_alim) equal to z_T when P_o is small (Almers, 1978; Sigg and Bezanilla, 1997). The limiting slope has been used to estimate z_T for K_V channels (Seoh et al., 1996; Islas and Sigworth, 1999) and Na⁺ channels (Hirschberg et al., 1995). However, for BK channels, the relationship between q_a and z_T is more complex because channels can open when no voltage sensors are activated (Horrigan and Aldrich, 2002). The mean P_o-V relation for mSlo1 in 0 Ca²⁺ is plotted on a semilog scale in Fig. 3 A and the corresponding q_a-V relation in Fig. 3 B. At extreme negative voltages (<–100 mV) P_o becomes very small (10^–7–10^–6) and weakly voltage dependent, exhibiting a limiting slope (q_aLim = 0.3 e; Fig. 3 A, dashed line) that represents the small charge associated with channel opening. At more positive voltages, q_a increases to a peak (q_aMAX = 1.9 ± 0.1 e) that reflects voltage sensor activation (Horrigan and Aldrich, 2002).

The relationship between q_a and z_T can be understood based on gating current measurements and some assumptions about voltage gating embodied in a model that accounts for BK channel gating in 0 Ca²⁺ (Fig. 3, C and D) (Horrigan et al., 1999). The HCA model postulates that the transition between the closed (C) and open (O) conformation is influenced allosterically by the state (resting [R] or activated [A]) of four independent and identical voltage sensors (Fig. 3 C). The energetic effect of voltage sensor activation on the C–O equilibrium is represented by a factor D and is fully described in terms of a two-tiered gating scheme (Fig. 3 D) representing the closed and open channel with different numbers (0–4) of activated voltage sensors. The equilibrium constants for the C–O and R–A transitions are both voltage dependent with partial charges z_L and z_J, respectively. Therefore the total gating charge involved in activating all four voltage sensors and opening the channel is z_T = (4z_J + z_L). z_J can be determined from the Q_C-V relation, which is measured from gating current when channels are closed and is well described by a Boltzmann function with a mean charge of z_J = 0.58 e (Horrigan and Aldrich, 2002). z_L can be determined from the limiting slope q_aLim = 0.3 e. Therefore, the estimated value of z_T = 2.62 e exceeds q_a at all voltages (Fig. 3 B). However the HCA model reproduces the P_o-V and q_a-V relations using these estimates of z_J, and z_L (Fig. 3, A and B, solid curves) and therefore reproduces the relationship between z_T and q_a.

In the present study we assessed the impact of mutations on z_T by measuring q_aMAX, and by fitting the P_o-V relations in various [Ca²⁺] with an expanded version of the HCA model that includes the effects of Ca²⁺ (Table I, HA model) (Horrigan and Aldrich, 2002). In principle, z_T could be estimated as for the WT channel, from gating currents and limiting slope. However, the expression of mutant channels was usually insufficient for gating current measurements. On the other hand, moderate levels of channel expression are sufficient to routinely measure the P_O-V relation and q_aMAX even at very low P_O, owing to the high single channel conductance of BK channels.

Although q_aMAX underestimates the total gating charge, simulations based on the HCA model imply that q_aMAX provides a reasonable indicator of changes in z_T. That is, the fractional change in q_aMAX for a mutant relative to the WT () approximates the fractional change in z_T () under most conditions. Fig. 3 E plots fq_aMAX versus fz_T as charge in the model is altered either by varying z_J alone or by varying z_J and z_L proportionally (solid lines). In both cases, a linear relationship is observed with a slope near unity, indicating that fq_aMAX approximates fz_T over a wide range of gating charge. q_aMAX is also sensitive to changes in the allosteric coupling factor D but is virtually unaffected by large changes in the equilibrium constants for voltage sensor activation (J₀) or channel opening (L₀) (Fig. 3 F). Examples of the effects on the P_o-V and q_a-V relations of altering the parameters z_J, L₀, J₀, or D individually are illustrated in Fig. 3 (G and H), respectively.

Distinguishing between Changes in Gating Charge and Allosteric Coupling
Because changes in q_aMAX may reflect changes in coupling (D) as well as changes in gating charge (z_J, z_L), it is important that we distinguish between these two possibilities. In general, we were able to determine which parameters in the HA model were altered by fitting the steady-state data (P_O and q_a) over a wide range of conditions. Many of the parameters are highly constrained by subsets of the data at extremes of voltage, [Ca²⁺], and P_O (Horrigan and Aldrich, 2002). When fitting these data we also focused on several features that depend specifically on coupling or charge. As described below, the magnitude of the P_o increase between extreme positive and negative voltages and the shape of the q_a-V relation provide direct indications of changes in coupling and charge respectively.

Allosteric coupling determines the extent to which the C–O equilibrium constant and P_O is increased by voltage sensor activation (Horrigan et al., 1999). Therefore changes in coupling should alter the magnitude of the P_O increase between extreme negative and positive voltages where voltage sensors are in the resting or activated state, respectively. For the WT channel in 0 Ca²⁺, P_O increases from a weakly voltage-dependent plateau near 10^–7 at extreme negative voltages to a level close to unity at voltages (+300 mV) where the Q-V relation is saturating and voltage sensors are fully activated (Horrigan and Aldrich, 1999). A simulated decrease in gating charge (z_J) that reduces q_aMAX by 35% has no effect on the magnitude of the P_O increase between extreme negative and positive voltages (Fig. 3 G, z_J). However, a decrease in coupling (D factor) that also reduces q_aMAX by 35% greatly inhibits the voltage-dependent P_O increase (Fig. 3 G, D). In this case, P_O fails to approach unity when voltage sensors are fully activated and instead achieves a plateau whose weak voltage dependence, like that at negative voltages, represents the charge associated with channel opening (z_L). Thus, decreases in coupling or charge should have effects on the P_O-V relation that are readily distinguishable, provided the resting and activated states of the voltage sensor are experimentally accessible, and P_o does not saturate before all voltage sensors are activated. Saturation could result from enhanced coupling (increased D factor) or stabilization of the open state (increased L₀) caused by mutation. Likewise, the presence of Ca²⁺ can obscure changes in coupling by stabilizing the open state.

Changes in gating charge have effects at negative voltages on the voltage dependence of q_a and P_O that are independent of changes in coupling. For any channel with multiple open states the q_a-V relation can be described as a function of P_O and the charge distributions (Q-V relations) for open and closed channels (Horrigan and Aldrich, 2002):

(2)

This function can be approximated by the difference of Q_O and Q_C when P_o is small:

(3)

when P_O << 1.

The relationship between gating charge and q_a defined by Eq. 3 is model independent and analogous to the limiting-slope analysis that has been applied to Shaker and other voltage-gated channels. In general, the shape and magnitude of Q_O-V and Q_C-V relations depend on gating charge, whereas coupling influences only their relative position along the voltage axis (Horrigan and Aldrich, 2002). Thus, Eq. 3 describes a bell-shaped function whose steepness is determined by charge and whose width is influenced by coupling. These properties can be defined exactly in the case of the HCA model, where both Q_O and Q_C are described by Boltzmann functions with identical voltage dependence but different half-activation voltages (V_HC and V_HO).

where

(4)

where

(5)

Combining Eqs. 3–5 yields an expression for q_a based on the HCA model:

(6)

when P_O << 1.

At extreme negative voltages q_a can be further approximated by Q_O (Eq. 5) (Horrigan and Aldrich, 2002). Fig. 3 B compares the voltage dependence of q_a from the HCA model (solid line) to that of Eqs. 5 and 6 (dashed lines). Eq. 6 provides a good approximation to the q_a-V relation near its peak and at more negative voltages, and therefore helps describe several properties of q_a. First, q_aMAX derived from Eq. 6 depends only on gating charge and coupling, as suggested by the simulations in Fig. 3 (E and F):

(7)

Second, the width of the q_a-V relation is related to the difference in half-activation voltages (V_H) between Q_O and Q_C and will therefore depend on both voltage sensor charge (z_J) and coupling (D):

(8)

Importantly, V_H has a reciprocal dependence on z_J and D that is distinct from that of q_aMAX. Therefore, decreases in charge or coupling that reduce q_aMAX will increase or decrease V_H, respectively, having opposite effects on the width of the q_a-V relation.

Simulations in Fig. 3 H demonstrate that decreases in D or z_J that have identical effects on q_aMAX have distinct effects on q_a-V shape. In addition to the opposing effects of D and z_J on q_a-V width, the steepness of q_a-V is altered by gating charge but is independent of coupling. In particular, the foot of the q_a-V relation is well approximated by Q_O (Fig. 3 B) and therefore has a voltage sensitivity that reflects only z_J and a voltage-independent component equal to z_L. In practice, measurements at the foot of the q_a-V relation for many mutants were noisy owing to the small amplitude of the corresponding P_O data. Therefore, to determine z_J, we took the approach of fitting q_a with the HCA model over a broader voltage range that includes q_aMAX. However, the fit was restricted to voltages where P_O < 0.1, satisfying the simplifying assumption in Eq. 6. In this way, fits depend on coupling as well as charge, but free parameters were limited and their effects could be distinguished based on the above analysis.

Effects of Voltage Sensor Mutations on Gating Charge and Coupling
The effects of individual S1–S4 mutations on gating charge were assessed by comparing fractional changes in the maximal logarithmic slope of the P_O-V relation (q_aMAX) (Fig. 4 A) to those in total gating charge (z_T) (Fig. 4 B) and coupling (D) (Fig. 4 C) estimated from fits to the allosteric models. Mutations at six positions in S2 (D153, R167), S3 (E180, D186), and S4 (R210, R213) reduced q_aMAX by significantly more than 10%. Four of these (D153, R167, D186, and R213) also reduced z_T and are potentially voltage sensing. Decreases in q_aMAX by R210E and E180A appear entirely accounted for by a reduction in the coupling factor D, whereas D186A reduces both charge and coupling.

The total gating charge (z_T = 4z_J + z_L) and coupling factor D were estimated by manual and semi-automated fitting protocols with similar results (solid and shaded bars in Fig. 4, B and C). The mean P_O-V, log(P_O)-V, and q_a-V relations in the presence and absence of Ca²⁺ were fit simultaneously using the HA model, with parameters adjusted manually (Table I) to provide the best fit by eye. The charge associated with the closed–open transition (z_L) was additionally constrained by the voltage dependence of (I_K), as described below. The dissociation constant for Ca²⁺ (K_D) and a weak interaction between voltage sensor activation and Ca²⁺ binding (allosteric factor E) have little impact on the determination of z_T or D and were held constant as a simplifying assumption (see Table I legend). Confidence intervals for z_T or D were estimated from the smallest change in z_J (Fig. 4 D) or D (Fig. 4 E) required to exceed the error range (SEM) of P_o. Because data was obtained over a wide range of P_O, V, and [Ca²⁺], using macroscopic and single channel methods, the parameters were well constrained, but we could not determine a satisfactory method of weighting the different data to allow automated fitting. We were able to fit the 0 Ca²⁺ data using a semi-automated procedure (see MATERIALS AND METHODS) that yielded values of z_T and D (Fig. 4, B and C, shaded bars) consistent with the manual estimates. Based on comparison of the mean and errors bars determined by these two methods a 10% change in z_T or q_aMAX or a 20% change in D were deemed significant.

Potential Voltage-sensing Residues in S2, S3, and S4
Steady-state data for mutants at the four potential voltage-sensing sites are compared with that of the WT in Figs. 5 and 6. Mean log(P_O)-V and q_a-V relations for the WT in 0–50 µM Ca²⁺ are plotted in Fig. 5 A and Fig. 6 A, respectively, together with fits to the HA model (solid lines). The corresponding data for R213C, D153K, R167E, and D186A in Fig. 5 (B–E) and Fig. 6 (B–E) are also fit with the HA model (solid lines) and compared with the WT fit (dashed lines). For the purpose of illustration, q_a is shown only in 0 Ca²⁺ and 50 µM Ca²⁺. However, it is evident from Fig. 5 that the maximal slope of the P_O-V relations (i.e., q_aMAX) for mutants were similarly reduced at all [Ca²⁺]. In addition, mutations increased the width and decreased the steepness of q_a-V relations, consistent with decreases in gating charge (Fig. 6).

View larger version (41K): [in this window] [in a new window]   Figure 5. Effect of potential voltage-sensing residue mutations on PO. Mean log(PO)-V relations for (A) WT, (B) R213C, (C) D153K, (D) R167A, and (E) D186A in 0–50 µM Ca2+. Solid lines are the fits to the HA model (Table I parameters). Dashed lines represent the WT fit. (F) Log(PO)-V relations in 0 Ca2+ for WT (), D153C(), D153K (), R213C (), R213E (), R167A (), R167E (), D186A(•), and R113Q () are superimposed to show that mutations reduce voltage dependence at the foot of the curve, consistent with a change in gating charge. Mutant curves were shifted along both axes as described below to match the WT at –90 mV. According to analysis presented in the text, the qa-V relation can be approximated by QO (Eq. 5) at extreme negative voltages. Therefore ln(PO) can be approximated as the sum of a linear and exponential function: ln(PO) = [ln(L0/(1 + L0))+(zL/kT)V] + [4DJ0exp(zJV/kT)]. Curves were shifted along the voltage axis such that the exponential component of this equation for all curves equaled 0.1 log unit at –90 mV, representing the transition between a linear and nonlinear function (i.e., the foot of the curve). Thus, the voltage shift for mutants was V = V0.1(WT) – V0.1(mutant) where V0.1= (kT/zJ)ln[0.1/(4DJ0log(e))], and the parameters zJ, D, and J0 were taken from Table I.

View larger version (40K): [in this window] [in a new window]   Figure 6. Effect of potential voltage-sensing residue mutations on qa. Mean qa-V relations for (A) WT, (B) R213C, (C) D153K, (D) R167A, and (E) D186A in 0 Ca2+ and 50 µM Ca2+. Solid lines are the fits to the HA model (Table I parameters). Dashed lines represent the WT fit. (F) Foot of the qa-V relations in 50 Ca2+ for WT (•), Y163E (), R213C (), D153K(), and R167A () are superimposed to show that the limiting value of qa (i.e., zL) is reduced by voltage sensor mutation. Dashed line represents zL for the WT (0.30 e).

The Location of Voltage-sensing Positions in S2
Two of the four potential voltage-sensing residues in mSlo1 are in S2 (D153, R167). K_V channels also contain conserved acidic and basic residues at these positions (Fig. 1 B). However, the residue corresponding to D153 in Shaker (E283) is non–voltage sensing (Seoh et al., 1996), and the functional role of that corresponding to R167 has not to our knowledge been reported. Shaker does have a potential voltage-sensing residue in S2 (E293) (Seoh et al., 1996) that corresponds to an uncharged residue in Slo1 (Y163) (Fig. 1 B). To determine if this position can sense voltage in mSlo1 we replaced it with the corresponding residue in Shaker (Y163E), but no significant change in q_aMAX or z_T was observed (Fig. 4, A and B; Table I). Thus the distribution of voltage-sensing and non–voltage-sensing positions in the S2 of BK and K_V channels appears to be different.

The Voltage Sensor Contributes to Charge Associated with Channel Opening (z_L)
The limiting slope of P_o at negative voltages (q_alim) represents the gating charge that moves when channels open (z_L) while voltage sensors are not activated (i.e., C₀–O₀ transition in HCA model; Fig. 3 D). The value of z_L for the WT (0.30 e, Table I) was determined as the slope of mean log(P_o) from –140 to –280 mV (50 µM Ca²⁺: z_L = 0.295 ± 0.012 [n = 10]; 5 µM Ca²⁺: z_L = 0.303 ± 0.021 [n = 3]) and confirms a previous estimate over a more limited voltage range (Horrigan and Aldrich, 2002). z_L is small and could result from subtle changes in the pore domain associated with channel opening, including redistribution of ions and the electric field within the pore (Jiang et al., 2002) or movement of charged residues that are present in S6. However, mutation of potential voltage-sensing residues in S2 (D153, R167) and S4 (R213) reduced z_L (Table I), suggesting that channel opening and voltage sensor activation share a common source of gating charge.

That z_L is reduced by voltage sensor mutation is evident by comparing the q_a-V relations of D153K, R167A, and R213C to that of the WT in 50 µM Ca²⁺ (Fig. 6 F). Over a range of negative voltages, q_a for these mutants is significantly less than the WT value of z_L (dashed line). A decrease in z_L is also obvious by comparing the limiting slope of the P_o-V relations for R167A (Fig. 6 D) to that of the WT fit (dashed lines). By contrast, mutation of a non–voltage-sensing residue (Y163E) shifted the q_a-V relation to more positive voltages relative to the WT but had no effect on q_alim (Fig. 6 F), indicating that z_L was unchanged. In the case of WT and Y163E channels, a limiting value of q_a was clearly achieved over a wide range of negative voltages, allowing z_L to be determined precisely. In general, however, z_L is difficult to determine because at the extreme voltages necessary to measure q_alim, steady-state recording for prolonged periods is problematic and P_O is small. Measurement error is minimized in 50 µM Ca²⁺ (e.g., Fig. 6 F) since P_O is increased more than 1,000-fold relative to 0 Ca²⁺ (Horrigan and Aldrich, 2002). However, in some cases, P_O could not be measured at sufficiently negative voltages to achieve a limiting slope (e.g., D186A; Fig. 6 E). More commonly, a limiting slope was achieved or closely approached but could not be measured over a wide enough voltage range to determine z_L within 0.1 e. By contrast, I_K deactivation kinetics can be measured over a much wider range of negative voltages (Horrigan and Aldrich, 2002). Therefore, the voltage dependence of (I_K) (Fig. 7) was used to estimate the values of z_L in Table I.

View larger version (27K): [in this window] [in a new window]   Figure 7. Voltage sensor mutations reduce the voltage dependence of channel closing. (A) Mean time constants of macroscopic IK ((IK)) for WT mSlo1 in 0 Ca2+() and 50 µM Ca2+() are plotted on a log scale versus voltage. The limiting exponential voltage dependence is indicated by a solid line that has a slope representing the partial charge zN for channel closing (0 Ca2+, 0.122 ± 0.002 e; 50 Ca2+, 0.130 ± 0.002 e). (B) (IK)-V relations in 50 µM Ca2+, normalized at –360 mV, for WT (), D153K (), R167A (), R213C (), and E219Q (). Lines are exponential fits. (C) zN for WT and mutants in 50 µM Ca2+ () is compared with the limiting slope of Po (qaLim) (). Starred symbols indicate values of zN that are significantly different from the WT (P < 0.0001, Student's t test).

Because z_N is easier to determine than the limiting slope of P_O, z_L for mutants (Table I) were usually estimated based on the fractional change in z_N relative to the WT:

(9)

A priori, the ratio of z_N to z_L need not remain constant. However, z_N and q_aLim were well correlated (r = 0.96) in cases where both were determined (Fig. 7 C), implying that Eq. 9 is a reasonable approximation. In one case (R167A), the fractional decrease in z_N was greater than the decrease in q_aLim; but this difference could reflect a failure to achieve a limiting value of q_a. For some mutants that behaved similar to the WT (R113Q, D133Q, and R210Q), z_N was not measured and z_L was set equal to the WT value. For mutations of R207 or R210, z_L was constrained by the voltage dependence of P_o at positive voltages as described below.

Effects of S4 Mutation on the Equilibrium Constant for Voltage Sensor Activation
Most mutations in S1–S4 shifted the P_o-V relation to more positive or negative voltages relative to the WT (Fig. 2 D), reflecting changes in the voltage sensor half-activation voltage (V_HC(J), Table I). V_HC(J) is a function of both voltage sensor charge (z_J) and the intrinsic stability of the activated state, represented by the zero-voltage equilibrium constant J₀ (i.e., V_HC(J) = –(kT/z_J) ln(J₀)). Thus, increases in V_HC(J) of up to several hundred millivolts produced by mutation of potential voltage-sensing residues R213 and D153 were largely accounted for by decreases in z_J, with little change in J₀ (Table I). By contrast, mutation of either R207 or R210 in S4 increased J₀ by several orders of magnitude without changing z_J, indicating that the stability of the activated state relative to the resting state was greatly enhanced. These effects on the energetics of voltage sensor activation show that non–voltage-sensing residues in S4 have an important impact on channel function.

Log(P_o)-V relations in 0 Ca²⁺ for the WT and several mutants that increase J_o (R207Q, R207E, and R210C) are compared in Fig. 8 A. An increase in J₀ shifts the steepest part of the curve to more negative voltages without altering its slope, as indicated by the HCA model fits (lines). This effect is most clearly demonstrated for R207Q and R207E because the steepest part of their log(P_O)-V relations can be measured, despite shifts of more than –200 mV in their position along the voltage axis relative to the WT. That charge neutralization (R207Q) and charge reversal (R207E) have virtually identical effects suggests that the removal of a positive charge at position 207 was critical for the increase in J₀. Gating current measurements confirm that mutation of R207Q enhances voltage sensor activation (Fig. 8 B) (Horrigan and Aldrich, 1999). The Q-V relation for R207Q, measured with admittance analysis (see MATERIALS AND METHODS) was shifted by –278 mV relative to the WT but is similar in shape, consistent with an increase in J_O with no change in z_J.

View larger version (42K): [in this window] [in a new window]   Figure 8. Effects of S4 mutation on the equilibrium for voltage sensor activation. (A) Mean log(PO)-V relations in 0 Ca2+ for WT(), R207Q (), R207E (), and R210C (). Mutant curves are shifted to more negative voltages, consistent with an increase in the equilibrium constant for voltage sensor activation (J0) in the HA model (lines, Table I parameters). (B) Normalized Q-V relations for WT and R207Q in 0 Ca2+ measured with admittance analysis from single experiments (see MATERIALS AND METHODS). Curves are fit with Boltzmann functions (WT: z = 0.59 e, Vh = 132 mV; R207Q: z = 0.65 e, Vh = –146 mV). (C) Po-V relations and fits from A are plotted on a linear scale to show that mutants have a similar PO and voltage dependence when voltage sensors are fully activated (i.e., V > 0). (D) qa-V relations for WT and R210C in 0 Ca2+ together with HA model fits showing that the voltage dependence of R210C is consistent with a gating charge similar to the WT. (E) Log(PO)-V relations for R210 mutants in 0 Ca2+ (R210C [], R210N [], R210E []). R210E was best fit at positive voltages by a Boltzmann function with a partial charge of 0.47 e (solid line). Dashed lines are Boltzmann functions with charge of 0.3 e, representing the value of zL for the WT. (F) (IK)-V relations for WT, R207Q, and R210C. Mutant curves are fit (lines) with a bell-shaped function (IK) = [4 + 4]–1 at potentials where voltage sensors are fully activated. 4 and 4 represent forward and backward rates for the C4–O4 transition in the HCA model (Fig. 3 D) and are exponentially dependent on voltage with partial charges z(4) and z(4), respectively.

In the case of R210C, P_O is weakly voltage dependent over a wide voltage range down to –200 mV (Fig. 8 A). A similar observation for R210N led Diaz et. al. (1998) to conclude that R210 is a voltage-sensing residue. However several lines of evidence indicate this is not the case. First, the P_o-V relations for R210C and R207Q are virtually identical at V > 0 (Fig. 8 C), implying that the voltage sensors of R210C, like R207Q, are fully activated. Second, when the voltage range of R210C was extended to –300 mV, the voltage dependence of P_O increased (Fig. 8 A). Although we could not make measurements at sufficiently negative voltages to determine q_aMAX, the q_a-V relation for R210C exhibits a steepness similar to that of the WT (Fig. 8 D), consistent with the assumption that z_J is unchanged (dashed fit). These observations suggest that R210C represents an extreme example of the effect represented by R207Q. That is, the voltage sensor equilibrium (J₀) for R210C is greatly increased such that the range of voltage sensor activation is shifted to extreme negative voltages, as indicated by the model fits in Fig. 8 (A and D). In this way, R210C appears weakly voltage dependent for V > –200 mV because voltage sensors are constitutively activated.

To confirm that R210 is non–voltage sensing, we examined the effects of additional mutations at this site (Fig. 8 E). Another charge-neutralizing mutation R210N exhibited reduced P_o relative to R210C, but a similar voltage dependence suggested that enhancement of voltage sensor activation does not require a cysteine residue. However a charge reversal (R210E) produced a qualitatively different effect than neutralization. First, the P_O-V relation of R210E appears less shifted than R210C and is strongly voltage dependent from –100 to +50 mV. Second, the magnitude of the P_O increase between extreme negative and positive voltages is greatly reduced relative to the WT, indicating a decrease in coupling between voltage sensor activation and channel opening (allosteric factor D). As discussed below, the P_o-V relation of R210E is consistent with a normal gating charge once changes in D are accounted for. Thus R210 is non–voltage sensing.

Voltage Sensor Activation May Increase the Charge Associated with Channel Opening
Based on the above results, we conclude that R207 and R210 are non–voltage sensing and do not contribute to z_J. However, the values of z_L determined for mutants at these positions appeared consistently larger than the WT (Table I). We do not think this represents a change in gating charge but rather a difference in the conditions under which z_L was determined. For mutants of R207 and R210, z_L was adjusted to fit the voltage dependence of P_O at positive voltages (e.g., Fig. 8 C) representing the charge to open the channel when voltage sensors are fully activated. For the WT and most mutants, z_L was determined from the voltage dependence of P_o and (I_K) at extreme negative voltages when voltage sensors are in the resting state. The difference in z_L might therefore be explained if the charge associated with channel opening is different when voltage sensors are in the resting or activated state. This hypothesis appears consistent with the P_o-V relation for R210E in 0 Ca (Fig. 8 E), representing the only mutant where the weak voltage dependence of P_O could be observed at both extreme positive and negative voltages. Boltzmann functions representing WT z_L (0.3 e, dashed lines) fit the P_O-V relation of R210E at negative voltages but not at positive voltages where the data are best fit with a charge of 0.47 e (solid line). Thus it appears that z_L increases when voltage sensors are activated.

To confirm the value of z_L for mutants of R207 and R210 we also examined the voltage dependence of (I_K) (Fig. 8 F). When voltage sensors are fully activated, channel gating in 0 Ca²⁺ should be approximated by a two-state model (C₄–O₄) and the (I_K)-V relation is described by bell-shaped function (I_K) = [₄+₄]^–1, where ₄ and ₄ represent the voltage-dependent forward and backward rate constants (Horrigan et al., 1999). The (I_K)-V relations for R207Q and R210C are well fit by this function (Fig. 8 F); and the summed partial charges associated with the forward and backward rates yield values from 0.34 to 0.58 e for different mutants (R207Q, 0.51 e; R207E, 0.58 e; R210C, 0.43 e; R210E, 0.34 e; R210N, 0.48 e). These estimates are comparable to values of z_L determine from P_o (Table I), but are probably not as accurate because the data must be fit at voltages near peak (I_K) where neither z(₄) nor z(₄) are well constrained.

Effects on Coupling between Voltage Sensor Activation and Channel Opening
Because decreases in the voltage dependence of P_o can be caused by decreases in allosteric coupling, we were careful to examine the effects of mutation on the coupling factor D. In most cases, large voltage-dependent increases in P_O were observed in 0 Ca²⁺, indicating that D was unchanged. However, three mutations (R210E, E180A, and D186A) reduced D significantly (Table I). Two of these in S3 (E180A, D186A) represent relatively small changes (twofold) that have a small impact on q_amax (<15%). By contrast, R210E exhibited a 30% reduction in q_amax that we attribute entirely to a sevenfold decrease in D.

Both R210E and E180A decreased the coupling factor D without altering gating charge. This is evident by comparing the log(P_O)-V relations of these mutants to the WT in 0 Ca²⁺ (Fig. 9 A). The foot of the curve for mutants and WT is superimposable, unlike mutants of potential voltage-sensing residues (Fig. 5 F), indicating that gating charge is not altered. However the magnitude of the voltage-dependent P_o increase is reduced relative to the WT, especially in the case of R210E. P_O-V relations for R210E in different [Ca²⁺] are plotted in Fig. 9 B together with fits to the WT data (dashed lines). The weak voltage dependence of R210E at both positive and negative voltages is consistent with complete activation and deactivation of voltage sensors, respectively. Between these extremes, P_o increases sharply over a 150 mV range like WT, consistent with a normal voltage sensor charge, but the magnitude of the P_o increase is roughly 1,000-fold smaller than WT. In 0 Ca²⁺, P_o for R210E is less than the WT at positive voltages but is 100-fold greater than the WT at extreme negative voltages. These differences can be reproduced with the HA model (solid lines) by a sevenfold reduction in D and a 100-fold increase in L_O. The reduction in D is necessary to account for the reduced magnitude of the voltage-dependent P_o increase and also accounts for the decrease in q_amax (Fig. 9 C). The q_a-V relation for R210E is narrower than that of the WT but has similar steepness at negative voltages, supporting the conclusion that coupling is reduced without altering gating charge.

View larger version (24K): [in this window] [in a new window]   Figure 9. Effects of voltage sensor mutations on coupling. (A) Mean log(PO)-V relations for WT (), E180A(), and R210E () in 0 Ca2+ are superimposed as in Fig. 5 F to show that mutations reduce the magnitude of the voltage-dependent PO increase without altering the voltage sensitivity of PO at negative voltages. (B) Mean log(PO)-V relations for R210E in 0–50 µM Ca2+. Solid lines are the fits to the HA model (Table I parameters) with the coupling factor D reduced sevenfold relative to the WT (dashed lines). (C) qa-v relations for R210E (•) and WT () in 0 Ca2+ with HA model fits. The similar voltage dependence of the foot of these curves show that gating charge (zJ, zL) is unchanged.